Optical image capturing system

ABSTRACT

A six-piece optical lens for capturing image and a six-piece optical module for capturing image are provided. In order from an object side to an image side, the optical lens along the optical axis includes a first lens with refractive power, a second lens with refractive power, a third lens with refractive power, a fourth lens with refractive power, a fifth lens with refractive power and a sixth lens with refractive power. At least one of the image-side surface and object-side surface of each of the six lens elements is aspheric. The optical lens can increase aperture value and improve the imagining quality for use in compact cameras.

CROSS-REFERENCE TO RELATED APPLICATION

This application claims the benefit of Taiwan Patent Application No.104126894, filed on Aug. 18, 2015, in the Taiwan Intellectual PropertyOffice, the disclosure of which is incorporated herein in its entiretyby reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present disclosure relates to an optical image capturing system, andmore particularly to a compact optical image capturing system which canbe applied to electronic products.

2. Description of the Related Art

In recent years, with the rise of portable electronic devices havingcamera functionalities, the demand for an optical image capturing systemis raised gradually. The image sensing device of ordinary photographingcamera is commonly selected from charge coupled device (CCD) orcomplementary metal-oxide semiconductor sensor (CMOS Sensor). Inaddition, as advanced semiconductor manufacturing technology enables theminimization of pixel size of the image sensing device, the developmentof the optical image capturing system directs towards the field of highpixels. Therefore, the requirement for high imaging quality is rapidlyraised.

The traditional optical image capturing system of a portable electronicdevice comes with different designs, including a four-lens or afifth-lens design. However, the requirement for the higher pixels andthe requirement for a large aperture of an end user, likefunctionalities of micro filming and night view have been raised. Theoptical image capturing system in prior arts cannot meet the requirementof the higher order camera lens module.

Therefore, how to effectively increase quantity of incoming light of theoptical lenses, and further improves imaging quality for the imageformation, becomes a quite important issue.

SUMMARY OF THE INVENTION

The aspect of embodiment of the present disclosure directs to an opticalimage capturing system and an optical image capturing lens which usecombination of refractive powers, convex and concave surfaces ofsix-piece optical lenses (the convex or concave surface in thedisclosure denotes the change of geometrical shape of an object-sidesurface or an image-side surface of each lens with different height froman optical axis) to increase the quantity of incoming light of theoptical image capturing system, and to improve imaging quality for imageformation, so as to be applied to minimized electronic products.

The term and its definition to the lens element parameter in theembodiment of the present invention are shown as below for furtherreference.

The Lens Element Parameter Related to a Length or a Height in the LensElement

A maximum height for image formation of the optical image capturingsystem is denoted by HOI. A height of the optical image capturing systemis denoted by HOS. A distance from the object-side surface of the firstlens element to the image-side surface of the sixth lens element isdenoted by InTL. A distance from an aperture stop (aperture) to an imageplane is denoted by InS. A distance from the first lens element to thesecond lens element is denoted by In12 (instance). A central thicknessof the first lens element of the optical image capturing system on theoptical axis is denoted by TP1 (instance).

The Lens Element Parameter Related to a Material in the Lens Element

An Abbe number of the first lens element in the optical image capturingsystem is denoted by NA1 (instance). A refractive index of the firstlens element is denoted by Nd1 (instance).

The Lens Element Parameter Related to a View Angle in the Lens Element

A view angle is denoted by AF. Half of the view angle is denoted by HAF.A major light angle is denoted by MRA.

The Lens Element Parameter Related to Exit/Entrance Pupil in the LensElement

An entrance pupil diameter of the optical image capturing system isdenoted by HEP. An entrance pupil diameter of the optical imagecapturing system is denoted by HEP. A maximum effective half diameterposition of any surface of single lens element means the vertical heightbetween the effective half diameter (EHD) and the optical axis where theincident light of the maximum view angle of the system passes throughthe farthest edge of the entrance pupil on the EHD of the surface of thelens element. For example, the maximum effective half diameter positionof the object-side surface of the first lens element is denoted asEHD11. The maximum effective half diameter position of the image-side ofthe first lens element is denoted as EHD12. The maximum effective halfdiameter position of the object-side surface of the second lens elementis denoted as EHD21. The maximum half effective half diameter positionof the image-side surface of the second lens element is denoted asEHD22. The maximum effective half diameter position of any surfaces ofthe remaining lens elements of the optical image capturing system can bereferred as mentioned above.

The Lens Element Parameter Related to an Arc Length of the Lens ElementShape and an Outline of Surface

A length of outline curve of the maximum effective half diameterposition of any surface of a single lens element refers to a length ofoutline curve from an axial point on the surface of the lens element tothe maximum effective half diameter position of the surface along anoutline of the surface of the lens element and is denoted as ARS. Forexample, the length of outline curve of the maximum effective halfdiameter position of the object-side surface of the first lens elementis denoted as ARS11. The length of outline curve of the maximumeffective half diameter position of the image-side surface of the firstlens element is denoted as ARS12. The length of outline curve of themaximum effective half diameter position of the object-side surface ofthe second lens element is denoted as ARS21. The length of outline curveof the maximum effective half diameter position of the image-sidesurface of the second lens element is denoted as ARS22. The lengths ofoutline curve of the maximum effective half diameter position of anysurface of the other lens elements in the optical image capturing systemare denoted in the similar way.

A length of outline curve of a half of an entrance pupil diameter (HEP)of any surface of a signal lens element refers to a length of outlinecurve of the half of the entrance pupil diameter (HEP) from an axialpoint on the surface of the lens element to a coordinate point ofvertical height with a distance of the half of the entrance pupildiameter from the optical axis on the surface along the outline of thesurface of the lens element and is denoted as ARE. For example, thelength of the outline curve of the half of the entrance pupil diameter(HEP) of the object-side surface of the first lens element is denoted asARE11. The length of the outline curve of the half of the entrance pupildiameter (HEP) of the image-side surface of the first lens element isdenoted as ARE12. The length of the outline curve of the half of theentrance pupil diameter (HEP) of the object-side surface of the secondlens element is denoted as ARE21. The length of the outline curve of thehalf of the entrance pupil diameter (HEP) of the image-side surface ofthe second lens element is denoted as ARE22. The lengths of outlinecurves of the half of the entrance pupil diameters (HEP) of any surfaceof the other lens elements in the optical image capturing system aredenoted in the similar way.

The Lens Element Parameter Related to a Depth of the Lens Element Shape

A horizontal distance in parallel with an optical axis from a maximumeffective half diameter position to an axial point on the object-sidesurface of the sixth lens element is denoted by InRS61 (a depth of themaximum effective half diameter). A horizontal distance in parallel withan optical axis from a maximum effective half diameter position to anaxial point on the image-side surface of the sixth lens element isdenoted by InRS62 (the depth of the maximum effective half diameter).The depths of the maximum effective half diameters (sinkage values) ofobject surfaces and image surfaces of other lens elements are denoted inthe similar way.

The Lens Element Parameter Related to the Lens Element Shape

A critical point C is a tangent point on a surface of a specific lenselement, and the tangent point is tangent to a plane perpendicular tothe optical axis and the tangent point cannot be a crossover point onthe optical axis. To follow the past, a distance perpendicular to theoptical axis between a critical point C51 on the object-side surface ofthe fifth lens element and the optical axis is HVT51 (instance). Adistance perpendicular to the optical axis between a critical point CS2on the image-side surface of the fifth lens element and the optical axisis HVT52 (instance). A distance perpendicular to the optical axisbetween a critical point C61 on the object-side surface of the sixthlens element and the optical axis is HVT61 (instance). A distanceperpendicular to the optical axis between a critical point C62 on theimage-side surface of the sixth lens element and the optical axis isHVT62 (instance). Distances perpendicular to the optical axis betweencritical points on the object-side surfaces or the image-side surfacesof other lens elements and the optical axis are denoted in the similarway described above.

The object-side surface of the sixth lens element has one inflectionpoint IF611 which is nearest to the optical axis, and the sinkage valueof the inflection point IF611 is denoted by SGI611. SGI611 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the object-side surface of the sixth lens element to theinflection point which is nearest to the optical axis on the object-sidesurface of the sixth lens element. A distance perpendicular to theoptical axis between the inflection point IF611 and the optical axis isHIF611 (instance). The image-side surface of the sixth lens element hasone inflection point IF621 which is nearest to the optical axis and thesinkage value of the inflection point IF621 is denoted by SGI621(instance). SGI621 is a horizontal shift distance in parallel with theoptical axis from an axial point on the image-side surface of the sixthlens element to the inflection point which is nearest to the opticalaxis on the image-side surface of the sixth lens element. A distanceperpendicular to the optical axis between the inflection point IF621 andthe optical axis is HIF621 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF612 which is the second nearest to the optical axis and thesinkage value of the inflection point IF612 is denoted by SGI612(instance). SGI612 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the second nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF612 and the optical axis is HIF612 (instance). The image-side surfaceof the sixth lens element has one inflection point IF622 which is thesecond nearest to the optical axis and the sinkage value of theinflection point IF622 is denoted by SGI622 (instance). SGI622 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the second nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF622 and the opticalaxis is HIF622 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF613 which is the third nearest to the optical axis and thesinkage value of the inflection point IF613 is denoted by SGI613(instance). SGI613 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the third nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF613 and the optical axis is HIF613 (instance). The image-side surfaceof the sixth lens element has one inflection point IF623 which is thethird nearest to the optical axis and the sinkage value of theinflection point IF623 is denoted by SGI623 (instance). SGI623 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the third nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF623 and the opticalaxis is HIF623 (instance).

The object-side surface of the sixth lens element has one inflectionpoint IF614 which is the fourth nearest to the optical axis and thesinkage value of the inflection point IF614 is denoted by SGI614(instance). SGI614 is a horizontal shift distance in parallel with theoptical axis from an axial point on the object-side surface of the sixthlens element to the inflection point which is the fourth nearest to theoptical axis on the object-side surface of the sixth lens element. Adistance perpendicular to the optical axis between the inflection pointIF614 and the optical axis is HIF614 (instance). The image-side surfaceof the sixth lens element has one inflection point IF624 which is thefourth nearest to the optical axis and the sinkage value of theinflection point IF624 is denoted by SGI624 (instance). SGI624 is ahorizontal shift distance in parallel with the optical axis from anaxial point on the image-side surface of the sixth lens element to theinflection point which is the fourth nearest to the optical axis on theimage-side surface of the sixth lens element. A distance perpendicularto the optical axis between the inflection point IF624 and the opticalaxis is HIF624 (instance).

The inflection points on the object-side surfaces or the image-sidesurfaces of the other lens elements and the distances perpendicular tothe optical axis thereof or the sinkage values thereof are denoted inthe similar way described above.

The Lens Element Parameter Related to an Aberration

Optical distortion for image formation in the optical image capturingsystem is denoted by ODT. TV distortion for image formation in theoptical image capturing system is denoted by TDT. Further, the range ofthe aberration offset for the view of image formation may be limited to50%-100%. An offset of the spherical aberration is denoted by DFS. Anoffset of the coma aberration is denoted by DFC.

The lateral aberration of the stop is denoted as STA to assess thefunction of the specific optical image capturing system. The tangentialfan or sagittal fan may be applied to calculate the STA of any viewfields, and in particular, to calculate the STA of the max referencewavelength (e.g. 650 nm) and the minima reference wavelength (e.g. 470nm) for serve as the standard of the optimal function. Theaforementioned direction of the tangential fan can be further defined asthe positive (overhead-light) and negative (lower-light) directions. Themax operation wavelength, which passes through the STA, is defined asthe image position of the specific view field, and the distancedifference of two positions of image position of the view field betweenthe max operation wavelength and the reference primary wavelength (e.g.wavelength of 555 nm), and the minimum operation wavelength, whichpasses through the STA, is defined as the image position of the specificview field, and STA of the max operation wavelength is defined as thedistance between the image position of the specific view field of maxoperation wavelength and the image position of the specific view fieldof the reference primary wavelength (e.g. wavelength of 555 nm), and STAof the minimum operation wavelength is defined as the distance betweenthe image position of the specific view field of the minimum operationwavelength and the image position of the specific view field of thereference primary wavelength (e.g. wavelength of 555 nm) are assessedthe function of the specific optical image capturing system to beoptimal. Both STA of the max operation wavelength and STA of the minimumoperation wavelength on the image position of vertical height with adistance from the optical axis to 70% HOI (i.e. 0.7 HOI), which aresmaller than 100 μm, are served as the sample. The numerical, which aresmaller than 80 μm, are also served as the sample.

A maximum height for image formation on the image plane perpendicular tothe optical axis in the optical image capturing system is denoted byHOI. A lateral aberration of the longest operation wavelength of avisible light of a positive direction tangential fan of the opticalimage capturing system passing through an edge of the entrance pupil andincident on the image plane by 0.7 HOI is denoted as PLTA. A lateralaberration of the shortest operation wavelength of a visible light ofthe positive direction tangential fan of the optical image capturingsystem passing through the edge of the entrance pupil and incident onthe image plane by 0.7 HOI is denoted as PSTA. A lateral aberration ofthe longest operation wavelength of a visible light of a negativedirection tangential fan of the optical image capturing system passingthrough the edge of the entrance pupil and incident on the image planeby 0.7 HOI is denoted as NLTA. A lateral aberration of the shortestoperation wavelength of a visible light of a negative directiontangential fan of the optical image capturing system passing through theedge of the entrance pupil and incident on the image plane by 0.7 HOI isdenoted as NSTA. A lateral aberration of the longest operationwavelength of a visible light of a sagittal fan of the optical imagecapturing system passing through the edge of the entrance pupil andincident on the image plane by 0.7 HOI is denoted as SLTA. A lateralaberration of the shortest operation wavelength of a visible light ofthe sagittal fan of the optical image capturing system passing throughthe edge of the entrance pupil and incident on the image plane by 0.7HOI is denoted as SSTA.

The disclosure provides an optical image capturing system, anobject-side surface or an image-side surface of the sixth lens elementmay have inflection points, such that the angle of incidence from eachview field to the sixth lens element can be adjusted effectively and theoptical distortion and the TV distortion can be corrected as well.Besides, the surfaces of the sixth lens element may have a betteroptical path adjusting ability to acquire better imaging quality.

The disclosure provides an optical image capturing system, in order froman object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. The first lenselement has refractive power. An object-side surface and an image-sidesurface of the sixth lens element are aspheric. Focal lengths of thefirst through sixth lens elements are f1, f2, f3, f4, f5 and f6respectively. A focal length of the optical image capturing system is f.An entrance pupil diameter of the optical image capturing system is HEP.A distance on an optical axis from an object-side surface of the firstlens element to the image plane is HOS. A distance on the optical axisfrom the object-side surface of the first lens element to the image-sidesurface of the sixth lens element is InTL. A length of outline curvefrom an axial point on any surface of any one of the six lens elementsto a coordinate point of vertical height with a distance of a half ofthe entrance pupil diameter from the optical axis on the surface alongan outline of the surface is denoted as ARE. The following relations aresatisfied: 1.2≦f/HEP≦10.0, 0<InTL/HOS<0.9, and 0.9≦2(ARE/HEP)≦1.5.

The disclosure provides another optical image capturing system, in orderfrom an object side to an image side, including a first, second, third,fourth, fifth, six lens elements and an image plane. The first lenselement has positive refractive power and may have a convex object-sidesurface near the optical axis. The second lens element has refractivepower. The third lens element has refractive power. The fourth lenselement has refractive power. The fifth lens element has refractivepower. The sixth lens element has refractive power and an object-sidesurface and an image-side surface of the sixth lens element areaspheric. At least two lens elements among the first through sixth lenselements respectively have at least one inflection point on at least onesurface thereof, and at least one of the first through fourth lenselements has positive refractive power. Focal lengths of the firstthrough sixth lens elements are f1, f2, f3, f4, f5 and f6 respectively.A focal length of the optical image capturing system is f. An entrancepupil diameter of the optical image capturing system is HEP. A distanceon an optical axis from an object-side surface of the first lens elementto the image plane is HOS. A distance on the optical axis from theobject-side surface of the first lens element to the image-side surfaceof the sixth lens element is InTL A length of outline curve from anaxial point on any surface of any one of the six lens elements to acoordinate point of vertical height with a distance of a half of theentrance pupil diameter from the optical axis on the surface along anoutline of the surface is denoted as ARE. The following relations aresatisfied: 1.2≦f/HEP≦10.0, 0<InTL/HOS<0.9, and 0.9≦2(ARE/HEP)≦1.5.

The disclosure provides another optical image capturing system, in orderfrom an object side to an image side, including a first, second, third,fourth, fifth, sixth lens elements and an image plane. At least onesurface among an object-side surface and an image-side surface of thesixth lens element has at least one inflection point. Wherein, theoptical image capturing system consists of the six lens elements withrefractive power. At least three lens elements among the first throughsixth lens elements respectively have at least one inflection point onat least one surface thereof. The first lens element has positiverefractive power. The second lens element has negative refractive power.The third lens element has refractive power. The fourth lens element hasrefractive power. The fifth lens element has refractive power. The sixthlens element has refractive power. Focal lengths of the first throughsixth lens elements are f1, f2, f3, f4, f5 and f6 respectively. A focallength of the optical image capturing system is f. An entrance pupildiameter of the optical image capturing system is HEP. A distance on anoptical axis from an object-side surface of the first lens element tothe image plane is HOS. A distance on the optical axis from theobject-side surface of the first lens element to the image-side surfaceof the sixth lens element is InTL A length of outline curve from anaxial point on any surface of any one of the six lens elements to acoordinate point of vertical height with a distance of a half of theentrance pupil diameter from the optical axis on the surface along anoutline of the surface is denoted as ARE. The following relations aresatisfied: 1.2≦f/HEP≦3.5, 0<InTL/HOS<0.9, and 0.9≦2(ARE/HEP)≦1.5.

The length of the outline curve of any surface of a signal lens elementin the maximum effective half diameter position affects the functions ofthe surface aberration correction and the optical path difference ineach view field. The longer outline curve may lead to a better functionof aberration correction, but the difficulty of the production maybecome inevitable. Hence, the length of the outline curve of the maximumeffective half diameter position of any surface of a signal lens element(ARS) has to be controlled, and especially, the ratio relations (ARS/TP)between the length of the outline curve of the maximum effective halfdiameter position of the surface (ARS) and the thickness of the lenselement to which the surface belongs on the optical axis (TP) has to becontrolled. For example, the length of the outline curve of the maximumeffective half diameter position of the object-side surface of the firstlens element is denoted as ARS11, and the thickness of the first lenselement on the optical axis is TP1, and the ratio between both of themis ARS11/TP1. The length of the outline curve of the maximum effectivehalf diameter position of the image-side surface of the first lenselement is denoted as ARS12, and the ratio between ARS12 and TP1 isARS12/TP1. The length of the outline curve of the maximum effective halfdiameter position of the object-side surface of the second lens elementis denoted as ARS21, and the thickness of the second lens element on theoptical axis is TP2, and the ratio between both of them is ARS21/TP2.The length of the outline curve of the maximum effective half diameterposition of the image-side surface of the second lens element is denotedas ARS22, and the ratio between ARS22 and TP2 is ARS22/TP2. The ratiorelations between the lengths of the outline curve of the maximumeffective half diameter position of any surface of the other lenselements and the thicknesses of the lens elements to which the surfacesbelong on the optical axis (TP) are denoted in the similar way.

The length of outline curve of half of an entrance pupil diameter of anysurface of a single lens element especially affects the functions of thesurface aberration correction and the optical path difference in eachshared view field. The longer outline curve may lead to a betterfunction of aberration correction, but the difficulty of the productionmay become inevitable. Hence, the length of outline curve of half of anentrance pupil diameter of any surface of a single lens element has tobe controlled, and especially, the ratio relationship between the lengthof outline curve of half of an entrance pupil diameter of any surface ofa single lens element and the thickness on the optical axis has to becontrolled. For example, the length of outline curve of the half of theentrance pupil diameter of the object-side surface of the first lenselement is denoted as ARE11, and the thickness of the first lens elementon the optical axis is TP1, and the ratio thereof is ARE11/TP1. Thelength of outline curve of the half of the entrance pupil diameter ofthe image-side surface of the first lens element is denoted as ARE12,and the thickness of the first lens element on the optical axis is TP1,and the ratio thereof is ARE12/TP1. The length of outline curve of thehalf of the entrance pupil diameter of the object-side surface of thefirst lens element is denoted as ARE21, and the thickness of the secondlens element on the optical axis is TP2, and the ratio thereof isARE21/TP2. The length of outline curve of the half of the entrance pupildiameter of the image-side surface of the second lens element is denotedas ARE22, and the thickness of the second lens element on the opticalaxis is TP2, and the ratio thereof is ARE22/TP2. The ratio relationshipof the remaining lens elements of the optical image capturing system canbe referred as mentioned above.

The height of optical system (HOS) may be reduced to achieve theminimization of the optical image capturing system when the absolutevalue of f1 is larger than f6 (|f1|>f6).

When |f2|+|f3|+|f4|+|f5| and |f1|+|f6| are satisfied with aboverelations, at least one of the second through fifth lens elements mayhave weak positive refractive power or weak negative refractive power.The weak refractive power indicates that an absolute value of the focallength of a specific lens element is greater than 10. When at least oneof the second through fifth lens elements has the weak positiverefractive power, the positive refractive power of the first lenselement can be shared, such that the unnecessary aberration will notappear too early. On the contrary, when at least one of the secondthrough fifth lens elements has the weak negative refractive power, theaberration of the optical image capturing system can be corrected andfine tuned.

The sixth lens element may have negative refractive power and a concaveimage-side surface. Hereby, the back focal length is reduced for keepingthe miniaturization, to miniaturize the lens element effectively. Inaddition, at least one of the object-side surface and the image-sidesurface of the sixth lens element may have at least one inflectionpoint, such that the angle of incident with incoming light from anoff-axis view field can be suppressed effectively and the aberration inthe off-axis view field can be corrected further.

BRIEF DESCRIPTION OF THE DRAWINGS

The detailed structure, operating principle and effects of the presentdisclosure will now be described in more details hereinafter withreference to the accompanying drawings that show various embodiments ofthe present disclosure as follows.

FIG. 1A is a schematic view of the optical image capturing systemaccording to the first embodiment of the present application.

FIG. 1B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the first embodimentof the present application.

FIG. 1C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the first embodiment of the presentapplication.

FIG. 2A is a schematic view of the optical image capturing systemaccording to the second embodiment of the present application.

FIG. 2B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the secondembodiment of the present application.

FIG. 2C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the second embodiment of the presentapplication.

FIG. 3A is a schematic view of the optical image capturing systemaccording to the third embodiment of the present application.

FIG. 3B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the third embodimentof the present application.

FIG. 3C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the third embodiment of the presentapplication.

FIG. 4A is a schematic view of the optical image capturing systemaccording to the fourth embodiment of the present application.

FIG. 4B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the fourthembodiment of the present application.

FIG. 4C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the fourth embodiment of the presentapplication.

FIG. 5A is a schematic view of the optical image capturing systemaccording to the fifth embodiment of the present application.

FIG. 5B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the fifth embodimentof the present application.

FIG. 5C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the fifth embodiment of the presentapplication.

FIG. 6A is a schematic view of the optical image capturing systemaccording to the sixth embodiment of the present application.

FIG. 6B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the sixth embodimentof the present application.

FIG. 6C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the sixth embodiment of the presentapplication.

FIG. 7A is a schematic view of the optical image capturing systemaccording to the seventh embodiment of the present application.

FIG. 7B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the seventhembodiment of the present application.

FIG. 7C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the seventh embodiment of the presentapplication.

FIG. 8A is a schematic view of the optical image capturing systemaccording to the eighth embodiment of the present application.

FIG. 8B is longitudinal spherical aberration curves, astigmatic fieldcurves, and an optical distortion grid of the optical image capturingsystem in the order from left to right according to the eighthembodiment of the present application.

FIG. 8C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the eighth embodiment of the presentapplication.

DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS

Reference will now be made in detail to the exemplary embodiments of thepresent disclosure, examples of which are illustrated in theaccompanying drawings. Therefore, it is to be understood that theforegoing is illustrative of exemplary embodiments and is not to beconstrued as limited to the specific embodiments disclosed, and thatmodifications to the disclosed exemplary embodiments, as well as otherexemplary embodiments, are intended to be included within the scope ofthe appended claims. These embodiments are provided so that thisdisclosure will be thorough and complete, and will fully convey theinventive concept to those skilled in the art. The relative proportionsand ratios of elements in the drawings may be exaggerated or diminishedin size for the sake of clarity and convenience in the drawings, andsuch arbitrary proportions are only illustrative and not limiting in anyway. The same reference numbers are used in the drawings and thedescription to refer to the same or like parts.

It will be understood that, although the terms ‘first’, ‘second’,‘third’, etc., may be used herein to describe various elements, theseelements should not be limited by these terms. The terms are used onlyfor the purpose of distinguishing one component from another component.Thus, a first element discussed below could be termed a second elementwithout departing from the teachings of embodiments. As used herein, theterm “or” includes any and all combinations of one or more of theassociated listed items.

An optical image capturing system, in order from an object side to animage side, includes a first, second, third, fourth, fifth and sixthlens elements with refractive power and an image plane. The opticalimage capturing system may further include an image sensing device whichis disposed on an image plane.

The optical image capturing system may use three sets of wavelengthswhich are 486.1 nm, 587.5 nm and 656.2 nm, respectively, wherein 587.5nm is served as the primary reference wavelength and a referencewavelength for retrieving technical features. The optical imagecapturing system may also use five sets of wavelengths which are 470 nm,510 nm, 555 nm, 610 nm and 650 nm, respectively, wherein 555 nm isserved as the primary reference wavelength and a reference wavelengthfor retrieving technical features.

A ratio of the focal length f of the optical image capturing system to afocal length fp of each of lens elements with positive refractive poweris PPR. A ratio of the focal length f of the optical image capturingsystem to a focal length fn of each of lens elements with negativerefractive power is NPR. A sum of the PPR of all lens elements withpositive refractive power is ΣPPR. A sum of the NPR of all lens elementswith negative refractive powers is ΣNPR. It is beneficial to control thetotal refractive power and the total length of the optical imagecapturing system when following conditions are satisfied:0.5≦ΣPPR/|ΣNPR|≦15. Preferably, the following relation may be satisfied:1≦ΣPPR/|ΣNPR|≦3.0.

The optical image capturing system may further include an image sensingdevice which is disposed on an image plane. Half of a diagonal of aneffective detection field of the image sensing device (imaging height orthe maximum image height of the optical image capturing system) is HOI.A on an optical axis distance on the optical axis from the object-sidesurface of the first lens element to the image plane is HOS. Thefollowing relations are satisfied: HOS/HOI≦10 and 0.5≦HOS/f≦10.Preferably, the following relations may be satisfied: 1≦HOS/HOI≦5 and1≦HOS/f≦7. Hereby, the miniaturization of the optical image capturingsystem can be maintained effectively, so as to be carried by lightweightportable electronic devices.

In addition, in the optical image capturing system of the disclosure,according to different requirements, at least one aperture stop may bearranged for reducing stray light and improving the imaging quality.

In the optical image capturing system of the disclosure, the aperturestop may be a front or middle aperture. The front aperture is theaperture stop between a photographed object and the first lens element.The middle aperture is the aperture stop between the first lens elementand the image plane. If the aperture stop is the front aperture, alonger distance between the exit pupil and the image plane of theoptical image capturing system can be formed, such that more opticalelements can be disposed in the optical image capturing system and theefficiency of receiving images of the image sensing device can beraised. If the aperture stop is the middle aperture, the view angle ofthe optical image capturing system can be expended, such that theoptical image capturing system has the same advantage that is owned bywide angle cameras. A distance from the aperture stop to the image planeis InS. The following relation is satisfied: 0.2≦InS/HOS≦1.1. Hereby,the miniaturization of the optical image capturing system can bemaintained while the feature of the wild-angle lens element can beachieved.

In the optical image capturing system of the disclosure, a distance fromthe object-side surface of the first lens element to the image-sidesurface of the sixth lens element is InTL. A total central thickness ofall lens elements with refractive power on the optical axis is ΣTP. Thefollowing relation is satisfied: 0.1≦TP/InTL≦0.9. Hereby, contrast ratiofor the image formation in the optical image capturing system anddefect-free rate for manufacturing the lens element can be givenconsideration simultaneously, and a proper back focal length is providedto dispose other optical components in the optical image capturingsystem.

A curvature radius of the object-side surface of the first lens elementis R1. A curvature radius of the image-side surface of the first lenselement is R2. The following relation is satisfied: 0.001≦|R1/R2|≦0.20.Hereby, the first lens element may have proper strength of the positiverefractive power, so as to avoid the longitudinal spherical aberrationto increase too fast. Preferably, the following relation may besatisfied: 0.01≦|R1/R2|<10.

A curvature radius of the object-side surface of the sixth lens elementis R11. A curvature radius of the image-side surface of the sixth lenselement is R12. The following relation is satisfied:−7<(R11−R12)/(R11+R12)<50. Hereby, the astigmatism generated by theoptical image capturing system can be corrected beneficially.

A distance between the first lens element and the second lens element onthe optical axis is IN12. The following relation is satisfied:IN12/f≦3.0. Hereby, the chromatic aberration of the lens elements can beimproved, such that the performance can be increased.

A distance between the fifth lens element and the sixth lens element onthe optical axis is IN56. The following relation is satisfied:IN56/f≦0.8. Hereby, the function of the lens elements can be improved.

Central thicknesses of the first lens element and the second lenselement on the optical axis are TP1 and TP2, respectively. The followingrelation is satisfied: 0.1≦(TP1+IN12)/TP2≦10. Hereby, the sensitivityproduced by the optical image capturing system can be controlled, andthe performance can be increased.

Central thicknesses of the fifth lens element and the sixth lens elementon the optical axis are TP5 and TP6, respectively, and a distancebetween the aforementioned two lens elements on the optical axis isIN56. The following relation is satisfied: 0.1≦(TP6+IN56)/TP5≦10.Hereby, the sensitivity produced by the optical image capturing systemcan be controlled and the total height of the optical image capturingsystem can be reduced.

Central thicknesses of the second lens element, the third lens elementand the fourth lens element on the optical axis are TP2, TP3 and TP4,respectively. A distance between the second and the third lens elementson the optical axis is IN23, and a distance between the third and thefourth lens elements on the optical axis is IN45. A distance between anobject-side surface of the first lens element and an image-side surfaceof sixth lens element is InTL. The following relation is satisfied:0.1≦TP4/(IN34+TP4+IN45)<1. Hereby, the aberration generated by theprocess of moving the incident light can be adjusted slightly layer uponlayer, and the total height of the optical image capturing system can bereduced.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C61on an object-side surface of the sixth lens element and the optical axisis HVT61. A distance perpendicular to the optical axis between acritical point C62 on an image-side surface of the sixth lens elementand the optical axis is HVT62. A distance in parallel with the opticalaxis from an axial point on the object-side surface of the sixth lenselement to the critical point C61 is SGC61. A distance in parallel withthe optical axis from an axial point on the image-side surface of thesixth lens element to the critical point C62 is SGC62. The followingrelations may be satisfied: 0 mm≦HVT61≦3 mm, 0 mm<HVT62≦6 mm,0≦HVT61/HVT62, 0 mm≦|SGC61|≦0.5 mm; 0 mm<|SGC62|≦2 mm, and0<|SGC62|/(|SGC62|+TP6)≦0.9. Hereby, the aberration of the off-axis viewfield can be corrected effectively.

The following relation is satisfied for the optical image capturingsystem of the disclosure: 0.2≦HVT62/HOI≦0.9. Preferably, the followingrelation may be satisfied: 0.3≦HVT62/HOI≦0.8. Hereby, the aberration ofsurrounding view field for the optical image capturing system can becorrected beneficially.

The following relation is satisfied for the optical image capturingsystem of the disclosure: 0≦HVT62/HOS≦0.5. Preferably, the followingrelation may be satisfied: 0.2≦HVT62/HOS≦0.45. Hereby, the aberration ofsurrounding view field for the optical image capturing system can becorrected beneficially.

In the optical image capturing system of the disclosure, a distance inparallel with an optical axis from an inflection point on theobject-side surface of the sixth lens element which is nearest to theoptical axis to an axial point on the object-side surface of the sixthlens element is denoted by SGI611. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesixth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the sixth lens element is denoted bySGI621. The following relations are satisfied: 0<SGI611/(SGI611+TP6)≦0.9and 0<SGI621/(SGI621+TP6)≦0.9. Preferably, the following relations maybe satisfied: 0.1≦SGI611/(SGI611+TP6)≦0.6 and0.1≦SGI621/(SGI621+TP6)≦0.6.

A distance in parallel with the optical axis from the inflection pointon the object-side surface of the sixth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the sixth lens element is denoted by SGI612. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the sixth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the sixth lenselement is denoted by SGI622. The following relations are satisfied:0<SGI612/(SGI612+TP6)≦0.9 and 0<SGI622/(SGI622+TP6)≦0.9. Preferably, thefollowing relations may be satisfied: 0.1≦SGI612/(SGI612+TP6)≦0.6 and0.1≦SGI622/(SGI622+TP6)≦0.6.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thenearest to the optical axis and the optical axis is denoted by HIF611. Adistance perpendicular to the optical axis between an axial point on theimage-side surface of the sixth lens element and an inflection point onthe image-side surface of the sixth lens element which is the nearest tothe optical axis is denoted by HIF621. The following relations aresatisfied: 0.001 mm≦|HIF611|≦5 mm and 0.001 mm≦|HIF621|≦5 mm.Preferably, the following relations may be satisfied: 0.1mm≦|HIF611|≦3.5 mm and 1.5 mm≦|HIF621|≦3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF612. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the second nearest to the optical axis is denoted by HIF622.The following relations are satisfied: 0.001 mm≦|HIF612|≦5 mm and 0.001mm≦|HIF622|≦5 mm. Preferably, the following relations may be satisfied:0.1 mm≦|HIF622|≦3.5 mm and 0.1 mm≦|HIF612|≦13.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF613. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the third nearest to the optical axis is denoted by HIF623. Thefollowing relations are satisfied: 0.001 mm≦|HIF613|≦5 mm and 0.001mm≦|HIF623|≦5 mm. Preferably, the following relations may be satisfied:0.1 mm≦|HIF623|≦3.5 mm and 0.1 mm≦|HIF613|≦3.5 mm.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF614. A distance perpendicular to the optical axis between an axialpoint on the image-side surface of the sixth lens element and aninflection point on the image-side surface of the sixth lens elementwhich is the fourth nearest to the optical axis is denoted by HIF624.The following relations are satisfied: 0.001 mm≦|HIF614|≦5 mm and 0.001mm≦|HIF624|≦5 mm. Preferably, the following relations may be satisfied:0.1 mm≦|HIF624|≦3.5 mm and 0.1 mm≦|HIF614|≦3.5 mm.

In one embodiment of the optical image capturing system of the presentdisclosure, the chromatic aberration of the optical image capturingsystem can be corrected by alternatively arranging the lens elementswith large Abbe number and small Abbe number.

The above Aspheric formula is:z=ch ²/[1+[1−(k+1)c ² h ²]^(0.5)]+A4h ⁴ +A6h ⁶ +A8h ⁸ +A10h ¹⁰ +A12h ¹²+A14h ¹⁴ +A16h ¹⁶ +A18h ¹⁸ +A20h ²⁰+ . . .  (1),where z is a position value of the position along the optical axis andat the height h which reference to the surface apex; k is the coniccoefficient, c is the reciprocal of curvature radius, and A4, A6, A8,A10, A12, A14, A16, A18, and A20 are high order aspheric coefficients.

The optical image capturing system provided by the disclosure, the lenselements may be made of glass or plastic material, if plastic materialis adopted to produce the lens elements, the cost of manufacturing willbe lowered effectively. If lens elements are made of glass, the heateffect can be controlled and the designed space arranged for therefractive power of the optical image capturing system can be increased.Besides, the object-side surface and the image-side surface of the firstthrough sixth lens elements may be aspheric, so as to obtain morecontrol variables. Comparing with the usage of traditional lens elementmade by glass, the number of lens elements used can be reduced and theaberration can be eliminated. Thus, the total height of the opticalimage capturing system can be reduced effectively.

In addition, in the optical image capturing system provided by thedisclosure, if the lens element has a convex surface, the surface of thelens element adjacent to the optical axis is convex in principle. If thelens element has a concave surface, the surface of the lens elementadjacent to the optical axis is concave in principle.

The optical image capturing system of the disclosure can be adapted tothe optical image capturing system with automatic focus if required.With the features of a good aberration correction and a high quality ofimage formation, the optical image capturing system can be used invarious application fields.

The optical image capturing system of the disclosure can include adriving module according to the actual requirements. The driving modulemay be coupled with the lens elements to enable the lens elementsproducing displacement. The driving module may be the voice coil motor(VCM) which is applied to move the lens to focus, or may be the opticalimage stabilization (OIS) which is applied to reduce the distortionfrequency owing to the vibration of the lens while shooting.

At least one of the first, second, third, fourth, fifth and sixth lenselements of the optical image capturing system of the disclosure mayfurther be designed as a light filtration element with a wavelength ofless than 500 n according to the actual requirement. The light filterelement may be made by coating at least one surface of the specific lenselement characterized of the filter function, and alternatively, may bemade by the lens element per se made of the material which is capable offiltering short wavelength.

According to the above embodiments, the specific embodiments withfigures are presented in detail as below.

The First Embodiment (Embodiment 1)

Please refer to FIG. 1A and FIG. 1B. FIG. 1A is a schematic view of theoptical image capturing system according to the first embodiment of thepresent application, FIG. 1B is longitudinal spherical aberrationcurves, astigmatic field curves, and an optical distortion curve of theoptical image capturing system in the order from left to right accordingto the first embodiment of the present application, and FIG. 1C is alateral aberration diagram of tangential fan, sagittal fan, the longestoperation wavelength and the shortest operation wavelength passingthrough an edge of the entrance pupil and incident on the image plane by0.7 HOI according to the first embodiment of the present application. Asshown in FIG. 1A, in order from an object side to an image side, theoptical image capturing system includes a first lens element 110, anaperture stop 100, a second lens element 120, a third lens element 130,a fourth lens element 140, a fifth lens element 150, a sixth lenselement 160, an IR-bandstop filter 180, an image plane 190, and an imagesensing device 192.

The first lens element 110 has negative refractive power and it is madeof plastic material. The first lens element 110 has a concaveobject-side surface 112 and a concave image-side surface 114, both ofthe object-side surface 112 and the image-side surface 114 are aspheric,and the object-side surface 112 has two inflection points. The length ofoutline curve of the maximum effective half diameter position of theobject-side surface of the first lens element is denoted as ARS11. Thelength of outline curve of the maximum effective half diameter positionof the image-side surface of the first lens element is denoted as ARS12.The length of outline curve of a half of an entrance pupil diameter(HEP) of the object-side surface of the first lens element is denoted asARE11, and the length of outline curve of the half of the entrance pupildiameter (HEP) of the image-side surface of the first lens element isdenoted as ARE12. The thickness of the first lens element on the opticalaxis is TP1.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the first lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefirst lens element is denoted by SGI111. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefirst lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the first lens element is denoted bySGI121. The following relations are satisfied: SGI111=−0.0031 mm and|SGI111|/(|SGI111|+TP1)=0.0016.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the first lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the first lens element is denoted by SGI112. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the first lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the first lenselement is denoted by SGI122. The following relations are satisfied:SGI112=1.3178 mm and |SGI112|/(|SGI112|+TP1)=0.4052.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the first lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefirst lens element is denoted by HIF111. A distance perpendicular to theoptical axis from the inflection point on the image-side surface of thefirst lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the first lens element is denoted byHIF121. The following relations are satisfied: HIF111=0.5557 mm andHIF111/HOI=0.1111.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the first lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the first lens element is denoted by HIF112. A distance perpendicularto the optical axis from the inflection point on the image-side surfaceof the first lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the first lenselement is denoted by HIF121. The following relations are satisfied:HIF112=5.3732 mm and HIF112/HOI=1.0746.

The second lens element 120 has positive refractive power and it is madeof plastic material. The second lens element 120 has a convexobject-side surface 122 and a convex image-side surface 124, and both ofthe object-side surface 122 and the image-side surface 124 are aspheric.The object-side surface 122 has an inflection point. The length ofoutline curve of the maximum effective half diameter position of theobject-side surface of the second lens element is denoted as ARS21, andthe length of outline curve of the maximum effective half diameterposition of the image-side surface of the second lens element is denotedas ARS22. The length of outline curve of a half of an entrance pupildiameter (HEP) of the object-side surface of the second lens element isdenoted as ARE21, and the length of outline curve of the half of theentrance pupil diameter (HEP) of the image-side surface of the secondlens element is denoted as ARE22. The thickness of the second lenselement on the optical axis is TP2.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the second lens element which is nearest tothe optical axis to an axial point on the object-side surface of thesecond lens element is denoted by SGI211. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesecond lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the second lens element is denoted bySGI221. The following relations are satisfied: SGI211=0.1069 mm,|SGI211|/(|SGI211|+TP2)=0.0412, SGI221=0 mm and|SGI221|/(|SGI221|++TP2)=0.

A distance perpendicular to the optical axis from the inflection pointon the object-side surface of the second lens element which is nearestto the optical axis to an axial point on the object-side surface of thesecond lens element is denoted by HIF211. A distance perpendicular tothe optical axis from the inflection point on the image-side surface ofthe second lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the second lens element is denoted byHIF221. The following relations are satisfied: HIF211=1.1264 mm,HIF211/HOI=0.2253, HIF221=0 mm and HIF221/HOI=0.

The third lens element 130 has negative refractive power and it is madeof plastic material. The third lens element 130 has a concaveobject-side surface 132 and a convex image-side surface 134, and both ofthe object-side surface 132 and the image-side surface 134 are aspheric.The object-side surface 132 and the image-side surface 134 both have aninflection point. The length of outline curve of the maximum effectivehalf diameter position of the object-side surface of the third lenselement is denoted as ARS31, and the length of outline curve of themaximum effective half diameter position of the image-side surface ofthe third lens element is denoted as ARS32. The length of outline curveof a half of an entrance pupil diameter (HEP) of the object-side surfaceof the third lens element is denoted as ARE31, and the length of outlinecurve of the half of the entrance pupil diameter (HEP) of the image-sidesurface of the third lens element is denoted as ARE32. The thickness ofthe third lens element on the optical axis is TP3.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the third lens element which is nearest tothe optical axis to an axial point on the object-side surface of thethird lens element is denoted by SGI311. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thethird lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the third lens element is denoted bySGI321. The following relations are satisfied: SGI311=−0.3041 mm,|SGI311|/(|SGI311|+TP3)=0.4445, SGI321=−0.1172 mm and|SGI321|/(|SGI321|+TP3)=0.2357.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the third lens element which isnearest to the optical axis and the optical axis is denoted by HIF311. Adistance perpendicular to the optical axis from the inflection point onthe image-side surface of the third lens element which is nearest to theoptical axis to an axial point on the image-side surface of the thirdlens element is denoted by HIF321. The following relations aresatisfied: HIF311=1.5907 mm, HIF311/HOI=0.3181, HIF321=1.3380 mm andHIF321/HOI=0.2676.

The fourth lens element 140 has positive refractive power and it is madeof plastic material. The fourth lens element 140 has a convexobject-side surface 142 and a concave image-side surface 144, both ofthe object-side surface 142 and the image-side surface 144 are aspheric,the object-side surface 142 has two inflection points, and theimage-side surface 144 has an inflection point. The length of outlinecurve of the maximum effective half diameter position of the object-sidesurface of the fourth lens element is denoted as ARS41, and the lengthof outline curve of the maximum effective half diameter position of theimage-side surface of the fourth lens element is denoted as ARS42. Thelength of outline curve of a half of an entrance pupil diameter (HEP) ofthe object-side surface of the fourth lens element is denoted as ARE41,and the length of outline curve of the half of the entrance pupildiameter (HEP) of the image-side surface of the fourth lens element isdenoted as ARE42. The thickness of the fourth lens element on theoptical axis is TP4.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fourth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefourth lens element is denoted by SGI411. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefourth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the fourth lens element is denoted bySGI421. The following relations are satisfied: SGI411=0.0070 mm,|SGI411|/(|SGI411|+TP4)=0.0056, SGI421=0.0006 mm and|SGI421|/(|SGI421|+TP4)=0.0005.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fourth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the fourth lens element is denoted by SGI412. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fourth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the fourth lenselement is denoted by SGI422. The following relations are satisfied:SGI412=−0.2078 mm and |SGI412|/(|SGI412|+TP4)=0.1439.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fourth lens element which isnearest to the optical axis and the optical axis is denoted by HIF411. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the fourth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF421. Thefollowing relations are satisfied: HIF411=0.4706 mm, HIF411/HOI=0.0941,HIF421=0.1721 mm and HIF421/HOI=0.0344.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fourth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF412. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fourth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF422. The following relations are satisfied: HIF412=2.0421mm and HIF412/HOI=0.4084.

The fifth lens element 150 has positive refractive power and it is madeof plastic material. The fifth lens element 150 has a convex object-sidesurface 152 and a convex image-side surface 154, and both of theobject-side surface 152 and the image-side surface 154 are aspheric. Theobject-side surface 152 has two inflection points and the image-sidesurface 154 has an inflection point. The length of outline curve of themaximum effective half diameter position of the object-side surface ofthe fifth lens element is denoted as ARS51, and the length of outlinecurve of the maximum effective half diameter position of the image-sidesurface of the fifth lens element is denoted as ARS52. The length ofoutline curve of a half of an entrance pupil diameter (HEP) of theobject-side surface of the fifth lens element is denoted as ARE51, andthe length of outline curve of the half of the entrance pupil diameter(HEP) of the image-side surface of the fifth lens element is denoted asARE52. The thickness of the fifth lens element on the optical axis isTP5.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thefifth lens element is denoted by SGI511. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thefifth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the fifth lens element is denoted bySGI521. The following relations are satisfied: SGI511=0.00364 mm,|SGI511|/(|SGI511|+TP5)=0.00338, SGI521=−0.63365 mm and|SGI521|/(|SGI521|+TP5)=0.37154.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI512. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the fifth lenselement is denoted by SGI522. The following relations are satisfied:SGI512=−0.32032 mm and |SGI512|/(|SGI512|+TP5)=0.23009.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the thirdnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI513. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the third nearest to the optical axisto an axial point on the image-side surface of the fifth lens element isdenoted by SGI523. The following relations are satisfied: SGI513=0 mm,|SGI513|/(|SGI513|+TP5)=0, SGI523=0 mm and |SGI523|/(|SGI523|+TP5)=0.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the fifth lens element which is the fourthnearest to the optical axis to an axial point on the object-side surfaceof the fifth lens element is denoted by SGI514. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the fifth lens element which is the fourth nearest to the opticalaxis to an axial point on the image-side surface of the fifth lenselement is denoted by SGI524. The following relations are satisfied:SGI514=0 mm, |SGI514|/(|SGI514|+TP5)=0, SGI524=0 mm and|SGI524|/(|SGI524|+TP5)=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which isnearest to the optical axis and the optical axis is denoted by HIF511. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the fifth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF521. Thefollowing relations are satisfied: HIF511=0.28212 mm,HIF511/HOI=0.05642, HIF521=2.13850 mm and HIF521/HOI=0.42770.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF512. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF522. The following relations are satisfied: HIF512=2.51384mm and HIF512, HOI=0.50277.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF513. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the third nearest to the optical axis and the optical axis isdenoted by HIF523. The following relations are satisfied: HIF513=0 mm,HIF513/HOI=0, HIF523=0 mm and HIF523/HOI=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the fifth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF514. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the fifth lens elementwhich is the fourth nearest to the optical axis and the optical axis isdenoted by HIF524. The following relations are satisfied: HIF514=0 mm,HIF514/HOI=0, HIF524=0 mm and HIF524/HOI=0.

The sixth lens element 160 has negative refractive power and it is madeof plastic material. The sixth lens element 160 has a concaveobject-side surface 162 and a concave image-side surface 164, and theobject-side surface 162 has two inflection points and the image-sidesurface 164 has an inflection point. Hereby, the angle of incident ofeach view field on the sixth lens element can be effectively adjustedand the spherical aberration can thus be improved. The length of outlinecurve of the maximum effective half diameter position of the object-sidesurface of the sixth lens element is denoted as ARS61, and the length ofoutline curve of the maximum effective half diameter position of theimage-side surface of the sixth lens element is denoted as ARS62. Thelength of outline curve of a half of an entrance pupil diameter (HEP) ofthe object-side surface of the sixth lens element is denoted as ARE61,and the length of outline curve of the half of the entrance pupildiameter (HEP) of the image-side surface of the sixth lens element isdenoted as ARE62. The thickness of the sixth lens element on the opticalaxis is TP6.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the sixth lens element which is nearest tothe optical axis to an axial point on the object-side surface of thesixth lens element is denoted by SGI611. A distance in parallel with anoptical axis from an inflection point on the image-side surface of thesixth lens element which is nearest to the optical axis to an axialpoint on the image-side surface of the sixth lens element is denoted bySGI621. The following relations are satisfied: SGI611=−0.38558 mm,|SGI611|/(|SGI611|+TP6)=0.27212, SGI621=0.12386 mm and|SGI621|/(|SGI621|+TP6)=0.10722.

A distance in parallel with an optical axis from an inflection point onthe object-side surface of the sixth lens element which is the secondnearest to the optical axis to an axial point on the object-side surfaceof the sixth lens element is denoted by SGI612. A distance in parallelwith an optical axis from an inflection point on the image-side surfaceof the sixth lens element which is the second nearest to the opticalaxis to an axial point on the image-side surface of the sixth lenselement is denoted by SGI622. The following relations are satisfied:SGI612=−0.47400 mm, |SGI612|/(|SGI612|+TP6)=0.31488, SGI622=0 mm and|SGI622|/(|SGI622|+TP6)=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which isnearest to the optical axis and the optical axis is denoted by HIF611. Adistance perpendicular to the optical axis between the inflection pointon the image-side surface of the sixth lens element which is nearest tothe optical axis and the optical axis is denoted by HIF621. Thefollowing relations are satisfied: HIF611=2.24283 mm,HIF611/HOI=0.44857, HIF621=1.07376 mm and HIF621/HOI=0.21475.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thesecond nearest to the optical axis and the optical axis is denoted byHIF612. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the second nearest to the optical axis and the optical axis isdenoted by HIF622. The following relations are satisfied: HIF612=2.48895mm and HIF612/HOI=0.49779.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thethird nearest to the optical axis and the optical axis is denoted byHIF613. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the third nearest to the optical axis and the optical axis isdenoted by HIF623. The following relations are satisfied: HIF613=0 mm,HIF613/HOI=0, HIF623=0 mm and HIF623/HOI=0.

A distance perpendicular to the optical axis between the inflectionpoint on the object-side surface of the sixth lens element which is thefourth nearest to the optical axis and the optical axis is denoted byHIF614. A distance perpendicular to the optical axis between theinflection point on the image-side surface of the sixth lens elementwhich is the fourth nearest to the optical axis and the optical axis isdenoted by HIF624. The following relations are satisfied: HIF614=0 mm,HIF614/HOI=0, HIF624=0 mm and HIF624/HOI=0.

The IR-bandstop filter 180 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 160 and the image plane 190.

In the optical image capturing system of the first embodiment, a focallength of the optical image capturing system is f, an entrance pupildiameter of the optical image capturing system is HEP, and half of amaximum view angle of the optical image capturing system is HAP. Thedetailed parameters are shown as below: f=4.075 mm, f/HEP=1.4,HAF=50.001 and tan(HAF)=1.1918.

In the optical image capturing system of the first embodiment, a focallength of the first lens element 110 is f1 and a focal length of thesixth lens element 160 is f6. The following relations are satisfied:f1=−7.828 mm, |f/f1|=0.52060, f6=−4.886 and |f1|>|f6|.

In the optical image capturing system of the first embodiment, focallengths of the second lens element 120 to the fifth lens element 150 aref2, f3, f4 and f5, respectively. The following relations are satisfied:|f2|f3|+|f4|+|f5|=95.50815 mm, |f1|+|f6|=12.71352 mm and|f2|+|f3|+|f4|+|f5|>|f1|+|f6|.

A ratio of the focal length f of the optical image capturing system to afocal length fp of each of lens elements with positive refractive poweris PPR. A ratio of the focal length f of the optical image capturingsystem to a focal length fn of each of lens elements with negativerefractive power is NPR. In the optical image capturing system of thefirst embodiment, a sum of the PPR of all lens elements with positiverefractive power is ΣPPR=f/f1+f3/f3+f/f5=1.63290. A sum of the NPR ofall lens elements with negative refractive powers isΣNPR=|f/f1|+|f/f3|+|f/f6|=1.51305, ΣPPR/|ΣNPR|=1.07921. The followingrelations are also satisfied: f/f2|=0.69101, |f/f3|=0.15834,|f/f4|=0.06883, |f/f5|=0.87305 and |f/f6|=0.83412.

In the optical image capturing system of the first embodiment, adistance from the object-side surface 112 of the first lens element tothe image-side surface 164 of the sixth lens element is InTL. A distancefrom the object-side surface 112 of the first lens element to the imageplane 190 is HOS. A distance from an aperture 100 to an image plane 190is InS. Half of a diagonal length of an effective detection field of theimage sensing device 192 is HOI. A distance from the image-side surface164 of the sixth lens element to the image plane 190 is BFL. Thefollowing relations are satisfied: InTL+BFL=HOS, HOS=19.54120 mm,HOI=5.0 mm, HOS/HOI=3.90824, HOS/f=4.7952, InS=11.685 mm andInS/HOS=0.59794.

In the optical image capturing system of the first embodiment, a totalcentral thickness of all lens elements with refractive power on theoptical axis is ΣTP. The following relations are satisfied: ΣTP=8.13899mm and ΣTP/InTL=0.52477. Hereby, contrast ratio for the image formationin the optical image capturing system and defect-free rate formanufacturing the lens element can be given considerationsimultaneously, and a proper back focal length is provided to disposeother optical components in the optical image capturing system.

In the optical image capturing system of the first embodiment, acurvature radius of the object-side surface 112 of the first lenselement is R1. A curvature radius of the image-side surface 114 of thefirst lens element is R2. The following relation is satisfied:|R1/R2|=8.99987. Hereby, the first lens element may have proper strengthof the positive refractive power, so as to avoid the longitudinalspherical aberration to increase too fast.

In the optical image capturing system of the first embodiment, acurvature radius of the object-side surface 162 of the sixth lenselement is R11. A curvature radius of the image-side surface 164 of thesixth lens element is R12. The following relation is satisfied:(R11−R12)/(R11+R12)=1.27780. Hereby, the astigmatism generated by theoptical image capturing system can be corrected beneficially.

In the optical image capturing system of the first embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=f2+f4+f5=69.770 mm andf5/(f2+f4+f5)=0.067. Hereby, it is favorable for allocating the positiverefractive power of the first lens element 110 to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=f1+f3+f6=−38.451 mm andf6/(f1+f3+f6)=0.127. Hereby, it is favorable for allocating the negativerefractive power of the sixth lens element 160 to other negative lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the first embodiment, adistance between the first lens element 110 and the second lens element120 on the optical axis is IN12. The following relations are satisfied:IN12=6.418 mm and IN12/f=1.57491. Hereby, the chromatic aberration ofthe lens elements can be improved, such that the performance can beincreased.

In the optical image capturing system of the first embodiment, adistance between the fifth lens element 150 and the sixth lens element160 on the optical axis is IN56. The following relations are satisfied:IN56=0.025 mm and IN56/f=0.00613. Hereby, the chromatic aberration ofthe lens elements can be improved, such that the performance can beincreased.

In the optical image capturing system of the first embodiment, centralthicknesses of the first lens element 110 and the second lens element120 on the optical axis are TP1 and TP2, respectively. The followingrelations are satisfied: TP1=1.934 mm, TP2=2.486 mm and(TP1+IN12)/TP2=3.36005. Hereby, the sensitivity produced by the opticalimage capturing system can be controlled, and the performance can beincreased.

In the optical image capturing system of the first embodiment, centralthicknesses of the fifth lens element 150 and the sixth lens element 160on the optical axis are TP5 and TP6, respectively, and a distancebetween the aforementioned two lens elements on the optical axis isIN56. The following relations are satisfied: TP5=1.072 mm, TP6=1.031 mmand (TP6+IN56)/TP5=0.98555. Hereby, the sensitivity produced by theoptical image capturing system can be controlled and the total height ofthe optical image capturing system can be reduced.

In the optical image capturing system of the first embodiment, adistance between the third lens element 130 and the fourth lens element140 on the optical axis is IN34. A distance between the fourth lenselement 140 and the fifth lens element 150 on the optical axis is IN45.The following relations are satisfied: IN34=0.401 mm, IN45=0.025 mm andTP4/(IN34+TP4+IN45)=0.74376. Hereby, the aberration generated by theprocess of moving the incident light can be adjusted slightly layer uponlayer, and the total height of the optical image capturing system can bereduced.

In the optical image capturing system of the first embodiment, adistance in parallel with an optical axis from a maximum effective halfdiameter position to an axial point on the object-side surface 152 ofthe fifth lens element is InRS51. A distance in parallel with an opticalaxis from a maximum effective half diameter position to an axial pointon the image-side surface 154 of the fifth lens element is InRS52. Acentral thickness of the fifth lens element 150 is TP5. The followingrelations are satisfied: InRS51=−0.34789 mm, InRS52=−0.88185 mm,|InRS51|/TP5=0.32458 and |InRS52|/TP5=0.82276. Hereby, it is favorablefor manufacturing and forming the lens element and for maintaining theminimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C51on the object-side surface 152 of the fifth lens element and the opticalaxis is HVT51. A distance perpendicular to the optical axis between acritical point C52 on the image-side surface 154 of the fifth lenselement and the optical axis is HVT52. The following relations aresatisfied: HVT51=0.515349 mm and HVT52=0 mm.

In the optical image capturing system of the first embodiment, adistance in parallel with an optical axis from a maximum effective halfdiameter position to an axial point on the object-side surface 162 ofthe sixth lens element is InRS61. A distance in parallel with an opticalaxis from a maximum effective half diameter position to an axial pointon the image-side surface 164 of the sixth lens element is InRS62. Acentral thickness of the sixth lens element 160 is TP6. The followingrelations are satisfied: InRS61=−0.58390 mm, InRS62=0.41976 mm,|InRS61|/TP6=0.56616 and |InRS62|/TP6=0.40700. Hereby, it is favorablefor manufacturing and forming the lens element and for maintaining theminimization for the optical image capturing system.

In the optical image capturing system of the first embodiment, adistance perpendicular to the optical axis between a critical point C61on the object-side surface 162 of the sixth lens element and the opticalaxis is HVT61. A distance perpendicular to the optical axis between acritical point C62 on the image-side surface 164 of the sixth lenselement and the optical axis is HVT62. The following relations aresatisfied: HVT61=0 mm and HVT62=0 mm.

In the optical image capturing system of the first embodiment, thefollowing relation is satisfied: HVT51/HOI=0.1031. Hereby, theaberration of surrounding view field can be corrected.

In the optical image capturing system of the first embodiment, thefollowing relation is satisfied: HVT51/HOS=0.02634. Hereby, theaberration of surrounding view field can be corrected.

In the optical image capturing system of the first embodiment, thesecond lens element 120, the third lens element 130 and the sixth lenselement 160 have negative refractive power. An Abbe number of the secondlens element is NA2. An Abbe number of the third lens element is NA3. AnAbbe number of the sixth lens element is NA6. The following relation issatisfied: NA6/NA2≦1. Hereby, the chromatic aberration of the opticalimage capturing system can be corrected.

In the optical image capturing system of the first embodiment, TVdistortion and optical distortion for image formation in the opticalimage capturing system are TDT and ODT, respectively. The followingrelations are satisfied: |TDT|=2.124% and |ODT|=5.076%.

In the optical image capturing system of the first embodiment, a lateralaberration of the longest operation wavelength of a visible light of apositive direction tangential fan of the optical image capturing systempassing through an edge of the aperture and incident on the image planeby 0.7 view field is denoted as PLTA, which is 0.006 mm. A lateralaberration of the shortest operation wavelength of a visible light ofthe positive direction tangential fan of the optical image capturingsystem passing through the edge of the aperture and incident on theimage plane by 0.7 view field is denoted as PSTA, which is 0.005 mm. Alateral aberration of the longest operation wavelength of a visiblelight of a negative direction tangential fan of the optical imagecapturing system passing through the edge of the aperture and incidenton the image plane by 0.7 view field is denoted as NLTA, which is 0.004mm. A lateral aberration of the shortest operation wavelength of avisible light of a negative direction tangential fan of the opticalimage capturing system passing through the edge of the aperture andincident on the image plane by 0.7 view field is denoted as NSTA, whichis −0.007 mm. A lateral aberration of the longest operation wavelengthof a visible light of a sagittal fan of the optical image capturingsystem passing through the edge of the aperture and incident on theimage plane by 0.7 view field is denoted as SLTA, which is −0.003 mm. Alateral aberration of the shortest operation wavelength of a visiblelight of the sagittal fan of the optical image capturing system passingthrough the edge of the aperture and incident on the image plane by 0.7view field is denoted as SSTA, which is 0.008 mm.

Please refer to the following Table 1 and Table 2.

The detailed data of the optical image capturing system of the firstembodiment is as shown in Table 1.

TABLE 1 Data of the optical image capturing system f = 4.075 mm, f/HEP =1.4, HAF = 50.000 deg Surface Focal # Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano Plano 1 Lens 1 −40.996257041.934 Plastic 1.515 56.55 −7.828 2 4.555209289 5.923 3 Ape. stop Plano0.495 4 Lens 2 5.333427366 2.486 Plastic 1.544 55.96 5.897 5−6.781659971 0.502 6 Lens 3 −5.697794287 0.380 Plastic 1.642 22.46−25.738 7 −8.883957518 0.401 8 Lens 4 13.19225664 1.236 Plastic 1.54455.96 59.205 9 21.55681832 0.025 10 Lens 5 8.987806345 1.072 Plastic1.515 56.55 4.668 11 −3.158875374 0.025 12 Lens 6 −29.46491425 1.031Plastic 1.642 22.46 −4.886 13 3.593484273 2.412 14 IR-bandstop Plano0.200 1.517 64.13 filter 15 Plano 1.420 16 Image plane Plano Referencewavelength (d-line) = 555 nm; shield position: The clear aperture of thefirst surface is 5.800 mm. The clear aperture of the third surface is1.570 mm. The clear aperture of the fifth surface is 1.950 mm.As for the parameters of the aspheric surfaces of the first embodiment,reference is made to Table 2.

TABLE 2 Aspheric Coefficients Surface # 1 2 4 5 6 7 8 k 4.310876E+01−4.707622E+00  2.616025E+00  2.445397E+00  5.645686E+00 −2.117147E+01−5.287220E+00 A4 7.054243E−03  1.714312E−02 −8.377541E−03 −1.789549E−02−3.379055E−03 −1.370959E−02 −2.937377E−02 A6 −5.233264E−04 −1.502232E−04 −1.838068E−03 −3.657520E−03 −1.225453E−03  6.250200E−03 2.743532E−03 A8 3.077890E−05 −1.359611E−04  1.233332E−03 −1.131622E−03−5.979572E−03 −5.854426E−03 −2.457574E−03 A10 −1.260650E−06  2.680747E−05 −2.390895E−03  1.390351E−03  4.556449E−03  4.049451E−03 1.874319E−03 A12 3.319093E−08 −2.017491E−06  1.998555E−03 −4.152857E−04−1.177175E−03 −1.314592E−03 −6.013661E−04 A14 −5.051600E−10  6.604615E−08 −9.734019E−04  5.487286E−05  1.370522E−04  2.143097E−04 8.792480E−05 A16 3.380000E−12 −1.301630E−09  2.478373E−04 −2.919339E−06−5.974015E−06 −1.399894E−05 −4.770527E−06 Surface # 9 10 11 12 13 k 6.200000E+01 −2.114008E+01 −7.699904E+00 −6.155476E+01 −3.120467E−01 A4−1.359965E−01 −1.263831E−01 −1.927804E−02 −2.492467E−02 −3.521844E−02 A6 6.628518E−02  6.965399E−02  2.478376E−03 −1.835360E−03  5.629654E−03 A8−2.129167E−02 −2.116027E−02  1.438785E−03  3.201343E−03 −5.466925E−04A10  4.396344E−03  3.819371E−03 −7.013749E−04 −8.990757E−04 2.231154E−05 A12 −5.542899E−04 −4.040283E−04  1.253214E−04 1.245343E−04  5.548990E−07 A14  3.768879E−05  2.280473E−05−9.943196E−06 −8.788363E−06 −9.396920E−08 A16 −1.052467E−06−5.165452E−07  2.898397E−07  2.494302E−07  2.728360E−09

The numerical related to the length of outline curve is shown accordingto table 1 and table 2.

First embodiment (Reference wavelength = 555 nm) ARE ½(HEP) ARE valueARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.455 1.455 −0.00033 99.98%1.934 75.23% 12 1.455 1.495 0.03957 102.72% 1.934 77.29% 21 1.455 1.4650.00940 100.65% 2.486 58.93% 22 1.455 1.495 0.03950 102.71% 2.486 60.14%31 1.455 1.486 0.03045 102.09% 0.380 391.02% 32 1.455 1.464 0.00830100.57% 0.380 385.19% 41 1.455 1.458 0.00237 100.16% 1.236 117.95% 421.455 1.484 0.02825 101.94% 1.236 120.04% 51 1.455 1.462 0.00672 100.46%1.072 136.42% 52 1.455 1.499 0.04335 102.98% 1.072 139.83% 61 1.4551.465 0.00964 100.66% 1.031 142.06% 62 1.455 1.469 0.01374 100.94% 1.031142.45% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 11 5.8006.141 0.341 105.88% 1.934 317.51% 12 3.299 4.423 1.125 134.10% 1.934228.70% 21 1.664 1.674 0.010 100.61% 2.486 67.35% 22 1.950 2.119 0.169108.65% 2.486 85.23% 31 1.980 2.048 0.069 103.47% 0.380 539.05% 32 2.0842.101 0.017 100.83% 0.380 552.87% 41 2.247 2.287 0.040 101.80% 1.236185.05% 42 2.530 2.813 0.284 111.22% 1.236 227.63% 51 2.655 2.690 0.035101.32% 1.072 250.99% 52 2.764 2.930 0.166 106.00% 1.072 273.40% 612.816 2.905 0.089 103.16% 1.031 281.64% 62 3.363 3.391 0.029 100.86%1.031 328.83%

Table 1 is the detailed structure data to the first embodiment in FIG.1A, wherein the unit of the curvature radius, the thickness, thedistance, and the focal length is millimeters (mm). Surfaces 0-16illustrate the surfaces from the object side to the image plane in theoptical image capturing system. Table 2 is the aspheric coefficients ofthe first embodiment, wherein k is the conic coefficient in the asphericsurface formula, and A1-A20 are the first to the twentieth orderaspheric surface coefficient. Besides, the tables in the followingembodiments are referenced to the schematic view and the aberrationgraphs, respectively, and definitions of parameters in the tables areequal to those in the Table 1 and the Table 2, so the repetitiousdetails will not be given here.

The Second Embodiment (Embodiment 2)

Please refer to FIG. 2A, FIG. 2B and FIG. 2C, FIG. 2A is a schematicview of the optical image capturing system according to the secondembodiment of the present application, FIG. 2B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the second embodiment of the present application, andFIG. 2C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the second embodiment of the presentapplication. As shown in FIG. 2A, in order from an object side to animage side, the optical image capturing system includes an aperture stop200, a first lens element 210, a second lens element 220, a third lenselement 230, a fourth lens element 240, a fifth lens element 250, asixth lens element 260, an IR-bandstop filter 280, an image plane 290,and an image sensing device 292.

The first lens element 210 has positive refractive power and it is madeof plastic material. The first lens element 210 has a convex object-sidesurface 212 and a convex image-side surface 214, and both of theobject-side surface 212 and the image-side surface 214 are aspheric. Theobject-side surface 212 has an inflection point.

The second lens element 220 has negative refractive power and it is madeof plastic material. The second lens element 220 has a convexobject-side surface 222 and a concave image-side surface 224, and bothof the object-side surface 222 and the image-side surface 224 areaspheric and have an inflection point.

The third lens element 230 has positive refractive power and it is madeof plastic material. The third lens element 230 has a convex object-sidesurface 232 and a convex image-side surface 234, and both of theobject-side surface 232 and the image-side surface 234 are aspheric. Theobject-side surface 232 has two infection points and the image-sidesurface 234 has an inflection point.

The fourth lens element 240 has negative refractive power and it is madeof plastic material. The fourth lens element 240 has a concaveobject-side surface 242 and a convex image-side surface 244, and both ofthe object-side surface 242 and the image-side surface 244 are aspheric.The object-side surface 242 has three inflection points and theimage-side surface 244 has an inflection point.

The fifth lens element 250 has positive refractive power and it is madeof plastic material. The fifth lens element 250 has a convex object-sidesurface 252 and a convex image-side surface 254, and both of theobject-side surface 252 and the image-side surface 254 are aspheric. Theobject-side surface 252 has two inflection points and the image-sidesurface 254 has three inflection points.

The sixth lens element 260 has negative refractive power and it is madeof plastic material. The sixth lens element 260 has a concaveobject-side surface 262 and a concave image-side surface 264. Hereby,the back focal length is reduced to miniaturize the lens elementeffectively. In addition, the object-side surface 262 has two inflectionpoints and the image-side surface 264 has an inflection point, such thatthe angle of incident with incoming light from an off-axis view fieldcan be suppressed effectively and the aberration in the off-axis viewfield can be corrected further.

The IR-bandstop filter 280 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 260 and the image plane 290.

In the optical image capturing system of the second embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=22.480 mm andf1/ΣPP=0.463. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the second embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−95.967 mm andf2/ΣNP=0.132. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 3 and Table 4.

The detailed data of the optical image capturing system of the secondembodiment is as shown in Table 3.

TABLE 3 Data of the optical image capturing system f = 5.908 mm; f/HEP =1.7; HAF = 40 deg Focal Surface # Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. stop Plano 0.000 2Lens 1 9.143553232 1.300 Plastic 1.544 55.96 10.399 3 −14.21076953 0.0004 Shading Plano 0.139 Sheet 5 Lens 2 3.883506563 0.350 Plastic 1.64222.46 −12.665 6 2.542254587 0.353 7 Lens 3 5.159333964 1.353 Plastic1.544 55.96 8.951 8 −83.45532538 0.635 9 Lens 4 −2.462872853 1.134Plastic 1.544 55.96 −80.463 10 −3.033307768 0.050 11 Lens 5 3.5773243740.475 Plastic 1.584 29.88 3.131 12 −3.598676562 0.221 13 Lens 6−11.83009685 0.888 Plastic 1.642 22.46 −2.838 14 2.240756706 0.822 15IR-bandstop Plano 0 200 BK_7 1.517 64.13 filter 16 Plano 1.500 17 Imageplane Plano Reference wavelength (d-line) = 555 nm; shield position:clear aperture (CA) of the fourth plano = 2.10 mmAs for the parameters of the aspheric surfaces of the second embodiment,reference is made to Table 4.

TABLE 4 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k  1.552658E+01−3.752184E+01  1.527900E+00 −7.410723E−02 −3.011631E+01 1.256090E+01−1.668609E+00 A4 −8.681658E−03 −2.322803E−02 −5.555401E−02 −5.570676E−02 1.187010E−02 3.225975E−03  2.996025E−02 A6  1.845993E−03  5.292353E−03 1.721085E−02  1.669248E−02 −9.782588E−03 −2.993131E−03  −1.098785E−02A8 −3.879186E−03 −3.181164E−03 −1.088565E−02 −8.449983E−03  4.653639E−031.278821E−03  3.071191E−03 A10  2.514534E−03  1.039589E−03  4.564600E−03 2.805240E−03 −1.872456E−03 −2.891801E−04  −2.038341E−04 A12−9.737351E−04 −1.714390E−04 −1.167692E−03 −5.944786E−04  4.062466E−042.589864E−05 −6.053170E−05 A14  1.992789E−04  9.461547E−06  1.635703E−04 7.065470E−05 −4.122732E−05 −1.450377E−06   1.056778E−05 A16−1.728027E−05  1.469456E−07 −1.003170E−05 −3.550150E−06  1.574765E−068.213400E−08 −4.639078E−07 Surface # 10 11 12 13 14 k −7.348841E+00 9.072380E−02 −4.061189E−01 −3.865251E+00 −3.123620E+00 A4 −8.888258E−02−2.278858E−02  1.621268E−01  8.553415E−02 −1.352540E−02 A6  4.089900E−02 1.306249E−02 −5.933169E−02 −3.784335E−02  1.472329E−03 A8 −1.245130E−02−5.960510E−03  1.308211E−02  9.288865E−03 −9.720593E−05 A10 2.447856E−03  1.295678E−03 −1.836109E−03 −1.340037E−03  3.150477E−06A12 −2.857855E−04 −1.605984E−04  1.564065E−04  1.123122E−04−1.463134E−08 A14  1.782840E−05  1.056885E−05 −7.376597E−06−5.087019E−06 −2.917720E−09 A16 −4.420350E−07 −2.818643E−07 1.483678E−07  9.627554E−08  7.864000E−11

In the second embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 3 and Table 4.

Second embodiment (Primary reference wavelength = 587.5 nm) |f/f1||f/f2| |f/f3| |f/f4| |f/f5| |f/f6| 0.56816 0.46648 0.66003 0.073421.88717 2.08139 ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN56/f TP4/(IN34 + TP4 +IN45) 3.11536 2.62130 1.18848 0.02359 0.03746 0.62352 |f1/f2| |f2/f3|(TP1 + IN12)/TP2 (TP6 + IN56)/TP5 0.82104 1.41491 4.11240 2.33790 HOSInTL HOS/HOI InS/HOS ODT % TDT % 9.41960 6.89803 1.88392 1.00000 1.030600.29832 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 2.13142 0    0.54845 3.40989 0.68198 0.36200 TP2/TP3 TP3/TP4 InRS61 InRS62|InRS61|/TP6 |InRS62|/TP6 0.25871 1.19321 0.10509 0.64670 0.118280.72788 PLTA PSTA NLTA NSTA SLTA SSTA −0.020 mm −0.020 mm 0.005 mm−0.015 mm 0.005 mm 0.008 mm

The numerical related to the length of outline curve is shown accordingto table 3 and table 4.

Second embodiment (Reference wavelength = 587.5 nm) ARE ½(HEP) ARE valueARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.738 1.740 0.00231 100.13%1.300 133.84% 12 1.738 1.774 0.03650 102.10% 1.300 136.47% 21 1.7381.745 0.00690 100.40% 0.350 498.44% 22 1.738 1.770 0.03230 101.86% 0.350505.70% 31 1.738 1.747 0.00935 100.54% 1.353 129.13% 32 1.738 1.737−0.00042 99.98% 1.353 128.41% 41 1.738 1.795 0.05775 103.32% 1.134158.35% 42 1.738 1.890 0.15187 108.74% 1.134 166.65% 51 1.738 1.7760.03854 102.22% 0.475 374.19% 52 1.738 1.758 0.02023 101.16% 0.475370.33% 61 1.738 1.746 0.00812 100.47% 0.888 196.49% 62 1.738 1.8030.06503 103.74% 0.888 202.90% ARS EHD ARS value ARS − EHD (ARS/EHD) % TPARS/TP (%) 11 1.739 1.741 0.00199 100.11% 1.300 133.92% 12 1.970 2.0500.07961 104.04% 1.300 157.69% 21 2.116 2.165 0.04963 102.35% 0.350618.68% 22 2.474 2.516 0.04164 101.68% 0.350 718.83% 31 2.649 2.6650.01549 100.58% 1.353 196.97% 32 2.788 2.913 0.12497 104.48% 1.353215.35% 41 2.826 2.919 0.09269 103.28% 1.134 257.44% 42 2.808 3.1490.34068 112.13% 1.134 277.70% 51 3.050 3.320 0.26921 108.83% 0.475699.33% 52 3.308 3.487 0.17833 105.39% 0.475 734.56% 61 3.453 3.5210.06816 101.97% 0.888 396.28% 62 4.113 4.244 0.13071 103.18% 0.888477.68%

The following contents may be deduced from Table 3 and Table 4.

Related inflection point values of second embodiment (Primary referencewavelength: 555 nm) HIF111 1.0544 HIF111/HOI 0.2109 SGI111 0.0533|SGI111|/(|SGI111| + TP1) 0.0394 HIF211 0.7721 HIF211/HOI 0.1544 SGI2110.0616 |SGI212|/(|SGI211| + TP2) 0.1497 HIF221 1.0730 HIF221/HOI 0.2146SGI221 0.1779 |SGI221|/(|SGI221| + TP2) 0.3370 HIF311 1.1388 HIF311/HOI0.2268 SGI311 0.1042 |SGI311|/(|SGI311| + TP3) 0.0715 HIF312 2.0806HIF312/HOI 0.4161 SGI312 0.1569 |SGI312|/(|SGI312| + TP3) 0.1039 HIF3212.6176 HIF321/HOI 0.5235 SGI321 −0.3506 |SGI321|/(|SGI321| + TP3) 0.2058HIF411 1.3612 HIF411/HOI 0.2722 SGI411 −0.2957 |SGI411|/(|SGI411| + TP4)0.2069 HIF412 2.0815 HIF412/HOI 0.4163 SGI412 −0.5094|SGI412|/(|SGI412| + TP4) 0.3100 HIF413 2.4715 HIF413/HOI 0.4943 SGI413−0.6158 |SGI413|/(|SGI413| + TP4) 0.3520 HIF421 1.9861 HIF421/HOI 0.3972SGI421 −0.8311 |SGI421|/(|SGI421| + TP4) 0.4230 HIF511 1.4412 HIF511/HOI0.2882 SGI511 0.2511 |SGI511|/(|SGI511| + TP5) 0.3460 HIF512 2.9541HIF512/HOI 0.5908 SGI512 −0.1037 |SGI512|/(|SGI512| + TP5) 0.1793 HIF5210.4109 HIF521/HOI 0.0822 SGI521 −0.0192 |SGI521|/(|SGI521| + TP5) 0.0388HIF522 1.7095 HIF522/HOI 0.3419 SGI522 0.1308 |SGI522|/(|SGI522| + TP5)0.2160 HIF523 3.2547 HIF523/HOI 0.6509 SGI523 −0.1207|SGI523|/(|SGI523| + TP5) 0.2027 HIF611 0.3015 HIF611/HOI 0.0603 SGI611−0.0032 |SGI611|/(|SGI611| + TP6) 0.0035 HIF612 2.2143 HIF612/HOI 0.4429SGI612 0.2105 |SGI612|/(|SGI612| + TP6) 0.1916

The Third Embodiment (Embodiment 3)

Please refer to FIG. 3A, FIG. 3B and FIG. 3C, FIG. 3A is a schematicview of the optical image capturing system according to the thirdembodiment of the present application, FIG. 3B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the third embodiment of the present application, andFIG. 3C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the third embodiment of the presentapplication. As shown in FIG. 3A, in order from an object side to animage side, the optical image capturing system includes an aperture stop300, a first lens element 310, a second lens element 320, a third lenselement 330, a fourth lens element 340, a fifth lens element 350, asixth lens element 360, an IR-bandstop filter 380, an image plane 390,and an image sensing device 392.

The first lens element 310 has positive refractive power and it is madeof plastic material. The first lens element 310 has a convex object-sidesurface 312 and a convex image-side surface 314, and both of theobject-side surface 312 and the image-side surface 314 are aspheric. Theobject-side surface 312 has an inflection point.

The second lens element 320 has negative refractive power and it is madeof plastic material. The second lens element 320 has a convexobject-side surface 322 and a concave image-side surface 324, and bothof the object-side surface 322 and the image-side surface 324 areaspheric and have an inflection point.

The third lens element 330 has positive refractive power and it is madeof plastic material. The third lens element 330 has a convex object-sidesurface 332 and a concave image-side surface 334, and both of theobject-side surface 332 and the image-side surface 334 are aspheric andhave two inflection points.

The fourth lens element 340 has negative refractive power and it is madeof plastic material. The fourth lens element 340 has a concaveobject-side surface 342 and a convex image-side surface 344, and both ofthe object-side surface 342 and the image-side surface 344 are asphericand have an inflection point.

The fifth lens element 350 has positive refractive power and it is madeof plastic material. The fifth lens element 350 has a convex object-sidesurface 352 and a convex image-side surface 354, and both of theobject-side surface 352 and the image-side surface 354 are aspheric. Theobject-side surface 352 has two inflection points and the image-sidesurface 354 has an inflection point.

The sixth lens element 360 has negative refractive power and it is madeof plastic material. The sixth lens element 360 has a convex object-sidesurface 362 and a concave image-side surface 364. Hereby, the back focallength is reduced to miniaturize the lens element effectively. Inaddition, the object-side surface 362 has two inflection points andimage-side surface 364 has an inflection point, such that the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 380 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 360 and the image plane 390.

In the optical image capturing system of the third embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=24.239 mm andf1/ΣPP=0.295. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the third embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−38.317 mm andf2/ΣNP=0.247. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 5 and Table 6.

The detailed data of the optical image capturing system of the thirdembodiment is as shown in Table 5.

TABLE 5 Data of the optical image capturing system f = 5.903 mm; f/HEP =1.9; HAF = 40 deg Focal Surface# Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. stop Plano 0.000 2Lens 1 8.488624861 1.300 Plastic 1.544 55.96 7.162 3 −6.852713513 0.0004 Shading Plano 0.206 Sheet 5 Lens 2 7.325343525 0.300 Plastic 1.64222.46 −9.476 6 3.285499885 0.473 7 Lens 3 7.220255188 1.162 Plastic1.544 55.96 13.531 8 305.205 0.453 9 Lens 4 −3.005750366 1.131 Plastic1.544 55.96 −25.124 10 −4.361067535 0.025 11 Lens 5 6.348885088 0.680Plastic 1.584 29.88 3.546 12 −2.977022761 0.209 13 Lens 6 11.741641831.117 Plastic 1.642 22.46 −3.718 14 1.923425401 0.772 15 IR-bandstopPlano 0.200 BK_7 1.517 64.13 filter 16 Plano 1.500 17 Image plane Plano0.000 Reference wavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the third embodiment,reference is made to Table 6.

TABLE 6 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k 1.988964E+01−5.691422E+00 8.409697E+00 5.393334E−01 −1.627552E+01  −1.802908E−04 −1.077835E−01  A4 −1.389285E−03  −1.076361E−02 −6.201521E−02 −7.171917E−02  −1.444273E−02  6.956247E−03 4.852580E−02 A6−1.019225E−02   3.766392E−03 2.912899E−02 2.614006E−02 2.699065E−04−1.917305E−02  −5.060293E−02  A8 1.057971E−02 −4.305212E−03−1.922216E−02  −1.141198E−02  −7.441999E−04  9.958992E−03 2.733693E−02A10 −7.502058E−03   1.381834E−03 8.105360E−03 2.974907E−03 9.385217E−05−2.967654E−03  −7.519023E−03  A12 2.823289E−03 −2.477427E−04−2.489938E−03  −5.177620E−04  3.883673E−05 4.720149E−04 1.112085E−03 A14−5.453225E−04   2.644413E−05 4.574517E−04 6.040088E−05 −7.373304E−06 −3.707166E−05  −8.355826E−05  A16 3.757486E−05 −2.306551E−06−3.626002E−05  −3.423159E−06  3.414247E−07 1.149031E−06 2.505886E−06 A180.000000E+00  0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A20 0.000000E+00  0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 Surface # 10 11 1213 14 k −2.471856E+01  2.533650E+00 −1.070255E−01 −8.998080E+01−3.332659E+00 A4 −1.596116E−01 −1.208191E−01  8.661858E−02  4.313250E−02−1.375647E−02 A6  7.782915E−02  6.107873E−02 −3.676763E−02 −2.521738E−02 1.056450E−03 A8 −2.548860E−02 −1.945542E−02  9.084662E−03  6.059937E−03 1.020157E−06 A10  5.789929E−03  3.845662E−03 −1.364045E−03−8.348822E−04 −8.490673E−06 A12 −8.216869E−04 −4.643019E−04 1.273213E−04  6.755965E−05  7.302147E−07 A14  6.389045E−05 3.093989E−05 −7.007254E−06 −2.994242E−06 −2.630087E−08 A16−2.050156E−06 −8.597551E−07  1.865574E−07  5.649823E−08  3.582600E−10

The presentation of the aspheric surface formula in the third embodimentis similar to that in the first embodiment. Besides, the definitions ofparameters in following tables are equal to those in the firstembodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 5 and Table 6.

Third embodiment (Primary reference wavelength: 555 nm) |f/f1| |f/f2||f/f3| |f/f4| |f/f5| |f/f6| 0.82421 0.62295 0.43623 0.23495 1.664731.58756 ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN56/f TP4/(IN34 + TP4 + TN45)2.92517 2.44545 1.19617 0.03488 0.03541 0.70309 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.75581 0.70027 5.01962 1.95185 HOS InTLHOS/HOI InS/HOS ODT % TDT % 9.52786 7.05542 1.90557 1.00000 0.949510.18632 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS  0.686461 0    1.76345 3.16641 0.63328 0.33233 TP2/TP3 TP3/TP4 InRS61 InRS62|InRS61|/TP6 |InRS62|/TP6 0.25817 1.02739 −0.34170  0.58545 0.305780.52391 PLTA PSTA NLTA NSTA SLTA SSTA −0.008 mm −0.015 mm 0.00044 mm−0.017 mm −0.002 mm 0.00011 mm

The numerical related to the length of outline curve is shown accordingto table 5 and table 6.

Third embodiment (Reference wavelength = 587.5 nm) ARE ½(HEP) ARE valueARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.553 1.557 0.00360 100.23%1.300 119.76% 12 1.553 1.584 0.03048 101.96% 1.300 121.83% 21 1.5531.565 0.01139 100.73% 0.300 521.58% 22 1.553 1.561 0.00774 100.50% 0.300520.36% 31 1.553 1.555 0.00166 100.11% 1.162 133.82% 32 1.553 1.5560.00245 100.16% 1.162 133.89% 41 1.553 1.607 0.05373 103.46% 1.131142.09% 42 1.553 1.684 0.13057 108.41% 1.131 148.88% 51 1.553 1.5580.00502 100.32% 0.680 229.30% 52 1.553 1.572 0.01891 101.22% 0.680231.35% 61 1.553 1.559 0.00612 100.39% 1.117 139.55% 62 1.553 1.6180.06418 104.13% 1.117 144.75% ARS EHD ARS value ARS − EHD (ARS/EHD) % TPARS/TP (%) 11 1.637 1.641 0.00380 100.23% 1.300 126.23% 12 1.949 2.0860.13666 107.01% 1.300 160.46% 21 1.997 2.175 0.17796 108.91% 0.300725.09% 22 2.376 2.454 0.07752 103.26% 0.300 818.00% 31 2.686 2.7100.02413 100.90% 1.162 233.20% 32 2.741 2.867 0.12642 104.61% 1.162246.75% 41 2.807 2.942 0.13508 104.81% 1.131 260.13% 42 2.827 3.1870.35954 112.72% 1.131 281.77% 51 2.922 3.041 0.11955 104.09% 0.680447.50% 52 3.004 3.167 0.16292 105.42% 0.680 465.99% 61 3.235 3.3400.10414 103.22% 1.117 298.85% 62 4.097 4.222 0.12513 103.05% 1.117377.79%

The following contents may be deduced from Table 5 and Table 6.

Related inflection point values of third embodiment (Primary referencewavelength: 555 nm) HIF111 1.1137 HIF111/HOI 0.2227 SGI111 0.0660|SGI111|/(|SGI111| + TP1) 0.0483 HIF211 0.5007 HIF211/HOI 0.1001 SGI2110.0138 |SGI211|/(|SGI211| + TP2) 0.0440 HIF221 0.7858 HIF221/HOI 0.1572SGI221 0.0735 |SGI221|/(|SGI221| + TP2) 0.1968 HIF311 0.7746 HIF311/HOI0.1549 SGI311 0.0346 |SGI311|/(|SGI311| + TP3) 0.0289 HIF312 1.9743HIF312/HOI 0.3949 SGI312 −0.0181 |SGI312|/(|SGI312| + TP3) 0.0153 HIF3210.4596 HIF321/HOI 0.0919 SGI321 0.0005 |SGI321|/(|SGI312| + TP3) 0.0004HIF322 2.3051 HIF322/HOI 0.4610 SGI322 −0.3824 |SGI322|/(|SGI322| + TP3)0.2476 HIF411 2.0433 HIF411/HOI 0.4087 SGI411 −0.5817|SGI411|/(|SGI411| + TP4) 0.3396 HIF421 1.7646 HIF421/HOI 0.3529 SGI421−0.7073 |SGI421|/(|SGI421| + TP4) 0.3848 HIF511 0.3611 HIF511/HOI 0.0722SGI511 0.0084 |SGI511|/(|SGI511| + TP5) 0.0122 HIF512 2.6313 HIF512/HOI0.5263 SGI512 −0.4603 |SGI512|/(|SGI512| + TP5) 0.4038 HIF521 2.6054HIF521/HOI 0.5211 SGI521 −0.6956 |SGI521|/(|SGI521| + TP5) 0.5058 HIF6111.1252 HIF611/HOI 0.2250 SGI611 0.0770 |SGI611|/(|SGI611| + TP6) 0.0645HIF612 3.1862 HIF612/HOI 0.6372 SGI612 −0.3120 |SGI612|/(|SGI612| + TP6)0.2183

The Fourth Embodiment (Embodiment 4)

Please refer to FIG. 4A, FIG. 4B and FIG. 4C, FIG. 4A is a schematicview of the optical image capturing system according to the fourthembodiment of the present application, FIG. 4B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the fourth embodiment of the present application, andFIG. 4C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the fourth embodiment of the presentapplication. As shown in FIG. 4A, in order from an object side to animage side, the optical image capturing system includes an aperture stop400, a first lens element 410, a second lens element 420, a third lenselement 430, a fourth lens element 440, a fifth lens element 450, asixth lens element 460, an IR-bandstop filter 480, an image plane 490,and an image sensing device 492.

The first lens element 410 has positive refractive power and it is madeof plastic material. The first lens element 410 has a convex object-sidesurface 412 and a convex image-side surface 414, and both of theobject-side surface 412 and the image-side surface 414 are aspheric. Theobject-side surface 412 has an inflection point.

The second lens element 420 has negative refractive power and it is madeof plastic material. The second lens element 420 has a convexobject-side surface 422 and a concave image-side surface 424, and bothof the object-side surface 422 and the image-side surface 424 areaspheric and have an inflection point.

The third lens element 430 has positive refractive power and it is madeof plastic material. The third lens element 430 has a convex object-sidesurface 432 and a concave image-side surface 434, and both of theobject-side surface 432 and the image-side surface 434 are aspheric. Theobject-side surface 432 has three inflection points and the image-sidesurface 434 has two inflection points.

The fourth lens element 440 has positive refractive power and it is madeof plastic material. The fourth lens element 440 has a concaveobject-side surface 442 and a convex image-side surface 444, and both ofthe object-side surface 442 and the image-side surface 444 are aspheric.The object-side surface 442 has two inflection points and the image-sidesurface 444 has an inflection point.

The fifth lens element 450 has positive refractive power and it is madeof plastic material. The fifth lens element 450 has a convex object-sidesurface 452 and a convex image-side surface 454, and both of theobject-side surface 452 and the image-side surface 454 are aspheric. Theobject-side surface 452 has an inflection point and the image-sidesurface 454 has three inflection points.

The sixth lens element 460 has negative refractive power and it is madeof plastic material. The sixth lens element 460 has a concaveobject-side surface 462 and a concave image-side surface 464. Hereby,the back focal length is reduced to miniaturize the lens elementeffectively. In addition, the object-side surface 462 has two inflectionpoints and the image-side surface 464 has an inflection point, such thatthe angle of incident with incoming light from an off-axis view fieldcan be suppressed effectively and the aberration in the off-axis viewfield can be corrected further.

The IR-bandstop filter 480 is made of plastic material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 460 and the image plane 490.

In the optical image capturing system of the fourth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=413.020 mm andf1/ΣPP=0.017. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the fourth embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−12.938 mm andf2/ΣNP=0.732. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 7 and Table 8.

The detailed data of the optical image capturing system of the fourthembodiment is as shown in Table 7.

TABLE 7 Data of the optical image capturing system f = 4.853 mm; f/HEP =1.7; HAF = 45 deg Focal Surface # Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. stop Plano 0.000 2Lens 1 17.61093889 1.300 Plastic 1.544 55.96 6.956 3 −4.713891104 0.0004 Shading Plano 0.130 Sheet 5 Lens 2 5.339522814 0.350 Plastic 1.64222.46 −9.468 6 2.78056208 0.323 7 Lens 3 7.306903102 0.789 Plastic 1.54455.96 8.579 8 −12.53571621 0.485 9 Lens 4 −1.958724362 1.285 Plastic1.544 55.96 394.017 10 −2.390488568 0.025 11 Lens 5 2.507805473 0.595Plastic 1.544 55.96 3.468 12 −7.073367628 0.364 13 Lens 6 −5.0818284570.448 Plastic 1.642 22.46 −3.470 14 4.16903487 0.725 15 IR-bandstopPlano 0.200 BK_7 1.517 64.13 filter 16 Plano 1.499 17 Image plane PlanoReference wavelength(d-line) = 555 nm, shield position: clear aperture(CA) of the fourth plano = 1.675 mmAs for the parameters of the aspheric surfaces of the fourth embodiment,reference is made to Table 8.

TABLE 8 Aspheric Coefficients Surface # 2 3 5 6 7 8 9 k  7.422000E−11−2.777007E+01  6.624231E+00  6.337866E−02 −6.947190E−01 −7.887069E−01−3.674780E−01 A4 −6.707218E−03 −1.457497E−02 −1.572678E−02 −3.986675E−02−2.924540E−02 −2.772931E−02  1.337101E−02 A6  1.365528E−03 −2.897936E−02−3.087097E−02  5.189410E−03  1.159449E−02  3.153416E−03  8.165527E−04 A8−6.258332E−03  2.873704E−02  1.311051E−02 −8.207930E−03 −3.301962E−03 2.434411E−03  3.772921E−03 A10  6.087025E−03 −1.670323E−02−2.405838E−03  5.556497E−03 −1.092131E−03 −7.959309E−04 −1.205663E−04A12 −3.425526E−03  5.815501E−03 −5.047540E−04 −1.976745E−03 8.119253E−04 −4.533094E−05 −4.300978E−04 A14  1.008759E−03−1.136863E−03  2.545168E−04  3.520008E−04 −1.492821E−04  4.718220E−05 1.021044E−04 A16 −1.272809E−04  9.402654E−05 −3.511814E−05−2.475658E−05  8.891886E−06 −4.776312E−06 −6.821594E−06 Surface # 10 1112 13 14 k −1.924300E−01 −1.694963E+00 4.183100E−10 −1.514100E−10−5.273200E−02 A4 −8.468603E−02  2.597001E−02 2.859859E−01  1.883591E−01 4.734293E−02 A6  5.870546E−02 −3.076164E−02 −1.666808E−01 −7.588630E−02 −2.306273E−02 A8 −2.035740E−02  9.823010E−03 5.178545E−02 1.595974E−02  4.151877E−03 A10  4.456296E−03 −1.396116E−03−9.554118E−03  −2.083287E−03 −3.988707E−04 A12 −5.741272E−04 5.155947E−05 1.032047E−03  1.747274E−04  2.114542E−05 A14  3.691003E−05 5.817970E−06 −6.013991E−05  −8.665735E−06 −5.811500E−07 A16−6.874752E−07 −4.453503E−07 1.455499E−06  1.890990E−07  6.327810E−09

The presentation of the aspheric surface formula in the fourthembodiment is similar to that in the first embodiment. Besides thedefinitions of parameters in following tables are equal to those in thefirst embodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 7 and Table 8.

Fourth embodiment (Primary reference wavelength: 587.5 nm) |f/f1| |f/f2||f/f3| |f/f4| |f/f5| |f/f6| 0.69759 0.51255 0.56568 0.01232 1.399131.39838 ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN56/f TP4/(IN34 + TP4 + IN45)2.19224 1.91094 1.14721 0.02674 0.07497 0.71600 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.73475 1.10365 4.08506 1.36322 HOS InTLHOS/HOI InS/HOS ODT % TDT % 8.51850 6.09388 1.70370 1.00000 2.545990.87395 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 2.19468 0    0.00000 3.11454 0.62291 0.36562 TP2/TP3 TP3/TP4 InRS61 InRS62|InRS61|/TP6 |InRS62|/TP6 0.44343 0.61447 −0.13164  0.27887 0.293860.62253 PLTA PSTA NLTA NSTA SLTA SSTA 0.001 mm 0.005 mm −0.022 mm 0.039mm 0.002 mm −0.001 mm

The numerical related to the length of outline curve is shown accordingto table 7 and table 8.

Fourth embodiment (Reference wavelength = 587.5 nm) ARE ½(HEP) ARE valueARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.427 1.428 0.00030 100.02%1.300 109.81% 12 1.427 1.465 0.03749 102.63% 1.300 112.67% 21 1.4271.432 0.00503 100.35% 0.350 409.23% 22 1.427 1.449 0.02130 101.49% 0.350413.88% 31 1.427 1.429 0.00136 100.09% 0.789 181.00% 32 1.427 1.4400.01246 100.87% 0.789 182.40% 41 1.427 1.519 0.09193 106.44% 1.285118.27% 42 1.427 1.561 0.13361 109.36% 1.285 121.51% 51 1.427 1.4810.05382 103.77% 0.595 248.72% 52 1.427 1.468 0.04031 102.82% 0.595246.45% 61 1.427 1.447 0.01994 101.40% 0.448 323.07% 62 1.427 1.4730.04526 103.17% 0.448 328.72% ARS EHD ARS value ARS − EHD (ARS/EHD) % TPARS/TP (%) 11 1.421 1.431 −0.00038 99.97% 1.300 110.04% 12 1.653 1.7310.07801 104.72% 1.300 133.12% 21 1.687 1.730 0.04264 102.53% 0.350494.20% 22 2.075 2.110 0.03455 101.66% 0.350 602.86% 31 2.249 2.2540.00457 100.20% 0.789 285.56% 32 2.351 2.395 0.04406 101.87% 0.789303.40% 41 2.355 2.523 0.16837 107.15% 1.285 196.43% 42 2.561 3.1180.55646 121.73% 1.285 242.70% 51 2.856 3.273 0.41688 114.59% 0.595549.67% 52 3.201 3.567 0.36576 111.43% 0.595 598.93% 61 3.422 3.6650.24279 107.09% 0.448 818.17% 62 4.096 4.410 0.31428 107.67% 0.448984.53%

The following contents may be deduced from Table 7 and Table 8.

Related inflection point values of fourth embodiment (Primary referencewavelength: 555 nm) HIF111 0.7358 HIF111/HOI 0.1472 SGI111 0.0133|SGI111|/(|SGI111| + TP1) 0.0101 HIF211 0.6861 HIF211/HOI 0.1372 SGI2110.0394 |SGI211|/(|SGI211| + TP2) 0.1013 HIF221 0.9541 HIF221/HOI 0.1908SGI221 0.1369 |SGI221|/(|SGI221| + TP2) 0.2812 HIF311 0.8010 HIF311/HOI0.1602 SGI311 0.0343 |SGI311|/(|SGI311| + TP3) 0.0417 HIF312 1.6666HIF312/HOI 0.3333 SGI312 0.0505 |SGI312|/(|SGI312| + TP3) 0.0601 HIF3132.1780 HIF313/HOI 0.4356 SGI313 0.0735 |SGI313|/(|SGI313| + TP3) 0.0852HIF321 1.7622 HIF321/HOI 0.3524 SGI321 −0.2510 |SGI321|/(|SGI321| + TP3)0.2413 HIF322 2.1928 HIF322/HOI 0.4386 SGI322 −0.3483|SGI322|/(|SGI322| + TP3) 0.3062 HIF411 1.2813 HIF411/HOI 0.2563 SGI411−0.39197 |SGI411|/(|SGI411| + TP4) 0.2338 HIF412 2.1976 HIF412/HOI0.4395 SGI412 −0.77843 |SGI412|/(|SGI412| + TP4) 0.3773 HIF421 2.2908HIF421/HOI 0.4582 SGI421 −1.34801 |SGI421|/(|SGI421| + TP4) 0.5121HIF511 1.2104 HIF511/HOI 0.2421 SGI511 0.2766 |SGI511|/(|SGI511| + TP5)0.3171 HIF521 0.2099 HIF521/HOI 0.0420 SGI521 −0.00257|SGI521|/(|SGI521| + TP5) 0.0043 HIF522 1.2924 HIF522/HOI 0.2585 SGI5220.2012 |SGI522|/(|SGI522| + TP5) 0.2526 HIF523 3.1056 HIF523/HOI 0.6211SGI523 −0.0959 |SGI523|/(|SGI523| + TP5) 0.1388 HIF611 0.3109 HIF611/HOI0.0622 SGI611 −0.0078 |SGI611|/(|SGI611| + TP6) 0.0172 HIF612 1.4050HIF612/HOI 0.2810 SGI612 0.1414 |SGI612|/(|SGI612| + TP6) 0.2400 HIF6211.4382 HIF621/HOI 0.2876 SGI621 0.3164 |SGI621|/(|SGI621| + TP6) 0.4139

The Fifth Embodiment (Embodiment 5)

Please refer to FIG. 5A, FIG. 5B and FIG. 5C, FIG. 5A is a schematicview of the optical image capturing system according to the fifthembodiment of the present application, FIG. 5B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the fifth embodiment of the present application, andFIG. 5C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the fifth embodiment of the presentapplication. As shown in FIG. 5A, in order from an object side to animage side, the optical image capturing system includes an aperture stop500, a first lens element 510, a second lens element 520, a third lenselement 530, a fourth lens element 540, a fifth lens element 550, asixth lens element 560, an IR-bandstop filter 580, an image plane 590,and an image sensing device 592.

The first lens element 510 has positive refractive power and it is madeof plastic material. The first lens element 510 has a convex object-sidesurface 512 and a convex image-side surface 514, and both of theobject-side surface 512 and the image-side surface 514 are aspheric. Theobject-side surface 512 has an inflection point.

The second lens element 520 has negative refractive power and it is madeof plastic material. The second lens element 520 has a convexobject-side surface 522 and a concave image-side surface 524, and bothof the object-side surface 522 and the image-side surface 524 areaspheric and have an inflection point.

The third lens element 530 has positive refractive power and it is madeof plastic material. The third lens element 530 has a convex object-sidesurface 532 and a convex image-side surface 534, and both of theobject-side surface 532 and the image-side surface 534 are aspheric andhave two inflection points.

The fourth lens element 540 has negative refractive power and it is madeof plastic material. The fourth lens element 540 has a concaveobject-side surface 542 and a convex image-side surface 544, and both ofthe object-side surface 542 and the image-side surface 544 are asphericand have an inflection point.

The fifth lens element 550 has positive refractive power and it is madeof plastic material. The fifth lens element 550 has a convex object-sidesurface 552 and a convex image-side surface 554, and both of theobject-side surface 552 and the image-side surface 554 are aspheric. Theobject-side surface 552 has an inflection point and the image-sidesurface 554 has two inflection points.

The sixth lens element 560 has negative refractive power and it is madeof plastic material. The sixth lens element 560 has a concaveobject-side surface 562 and a concave image-side surface 564. Hereby,the back focal length is reduced to miniaturize the lens elementeffectively. In addition, the object-side surface 562 has two inflectionpoints and the image-side surface 564 has an inflection point, such thatthe angle of incident with incoming light from an off-axis view fieldcan be suppressed effectively and the aberration in the off-axis viewfield can be corrected further.

The IR-bandstop filter 580 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 560 and the image plane 590.

In the optical image capturing system of the fifth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relation is satisfied: ΣPP=15.501 mm andf1/ΣPP=0.377. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the fifth embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relation is satisfied: ΣNP=−31.075 mm andf2/ΣNP=0.260. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 9 and Table 10.

The detailed data of the optical image capturing system of the fifthembodiment is as shown in Table 9.

TABLE 9 Data of the optical image capturing system f = 4.910 mm; f/HEP =1.9; HAF = 45 deg Focal Surface # Curvature Radius Thickness MaterialIndex Abbe # length 0 Object Plano At infinity 1 Ape. stop Plano 0.000 2Lens 1 7.344381711 0.721 Plastic 1.544 55.96 5.850 3 −5.451474742 0.0304 Lens 2 4.490345605 0.350 Plastic 1.642 22.46 −8.073 5 2.3416102650.460 6 Lens 3 45.40359813 0.840 Plastic 1.544 55.96 6.100 7−3.569081412 0.662 8 Lens 4 −1.124568132 0.779 Plastic 1.544 55.96−19.465 9 −1.565224199 0.025 10 Lens 5 2.872859215 0.905 Plastic 1.54455.96 3.551 11 −5.29436343 0.049 12 Lens 6 −37.95881249 0.638 Plastic1.642 22.46 −3.538 13 2.454687075 0.625 14 IR-bandstop Plano 0.200 BK_71.517 64.13 filter 15 Plano 1.500 16 Image plane Plano Referencewavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the fifth embodiment,reference is made to Table 10.

TABLE 10 Aspheric Coefficients Surface # 2 3 5 6 7 8 k 3.311714E+00−8.961284E+00 1.877474E+00 −8.394291E−02 0.000000E+00 −1.298539E+01 A4−5.495021E−03 1.146268E−02 −4.227878E−02 −8.235417E−02 −1.363984E−02−4.345523E−02 A6 −1.384949E−02 1.070219E−03 3.795785E−02 5.756723E−02−4.234894E−03 1.072202E−02 A8 1.691272E−02 −3.795938E−02 −4.810827E−02−4.348221E−02 6.667845E−03 −6.251270E−03 A10 −1.652625E−02 4.110200E−023.230425E−02 2.059555E−02 −3.937396E−03 4.680449E−03 A12 8.700336E−03−2.247561E−02 −1.281029E−02 −6.140966E−03 1.301987E−03 −1.285248E−03 A14−2.500727E−03 6.221046E−03 2.678449E−03 1.004570E−03 −2.049518E−041.481428E−04 A16 2.822365E−04 −6.991077E−04 −2.258674E−04 −6.742795E−051.196264E−05 −6.255894E−06 Surface # 9 10 11 12 13 14 k −1.530066E+00−5.010684E+00 −1.296138E−01 0.000000E+00 0.000000E+00 −9.447198E+00 A41.029136E−01 −5.051552E−02 −2.340000E−02 1.226866E−01 7.826066E−021.926049E−02 A6 −1.194601E−01 −1.351367E−02 −3.510227E−02 −7.036463E−02−3.381080E−02 −7.258561E−03 A8 7.095001E−02 1.477214E−02 2.021912E−022.186762E−02 7.947217E−03 1.081827E−03 A10 −2.054184E−02 −3.972939E−03−5.356646E−03 −4.022903E−03 −1.250192E−03 −9.387930E−05 A12 3.192280E−034.507212E−04 7.710988E−04 4.347314E−04 1.266591E−04 4.753602E−06 A14−2.574548E−04 −1.313442E−05 −5.877236E−05 −2.562642E−05 −7.450247E−06−1.298179E−07 A16 8.511117E−06 −5.641216E−07 1.846182E−06 6.314398E−071.885900E−07 1.450460E−09

The presentation of the aspheric surface formula in the fifth embodimentis similar to that in the first embodiment. Besides the definitions ofparameters in following tables are equal to those in the firstembodiment so the repetitious details will not be given here.

The following contents may be deduced from Table 9 and Table 10.

Fifth embodiment (Primary reference wavelength: 587.5 nm) |f/f1| |f/f2||f/f3| |f/f4| |f/f5| |f/f6| 0.83939 0.60822 0.80494 0.25225 1.382621.38776 ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN56/f TP4/(IN34 + TP4 + IN45)3.02695 2.24824 1.34637 0.00614 0.00995 0.53129 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.72460 1.32343 2.14733 0.75817 HOS InTLHOS/HOI InS/HOS ODT % TDT % 7.78387 5.45928 1.55677 1.00000 2.500220.67322 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 1.64556 0    0.00000 2.68615 0.53723 0.34509 TP2/TP3 TP3/TP4 InRS61 InRS62|InRS61|/TP6 |InRS62|/TP6 0.41652 1.07902 −0.46895  0.03796 0.735540.05954 PLTA PSTA NLTA NSTA SLTA SSTA 0.014 mm 0.013 mm 0.00048 mm−0.011 mm 0.016 mm 0.010 mm

The numerical related to the length of outline curve is shown accordingto table 9 and table 10.

Fifth embodiment (Reference wavelength = 555 nm) ARE ½(HEP) ARE valueARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.292 1.294 0.00231 100.18%0.721 179.42% 12 1.292 1.308 0.01624 101.26% 0.721 181.35% 21 1.2921.297 0.00532 100.41% 0.350 370.69% 22 1.292 1.321 0.02896 102.24% 0.350377.45% 31 1.292 1.292 0.00030 100.02% 0.840 153.80% 32 1.292 1.3280.03547 102.74% 0.840 157.99% 41 1.292 1.434 0.14218 111.00% 0.779184.17% 42 1.292 1.409 0.11643 109.01% 0.779 180.87% 51 1.292 1.3060.01412 101.09% 0.905 144.28% 52 1.292 1.293 0.00044 100.03% 0.905142.77% 61 1.292 1.298 0.00563 100.44% 0.638 203.55% 62 1.292 1.3260.03353 102.59% 0.638 207.92% ARS EHD ARS value ARS − EHD (ARS/EHD) % TPARS/TP (%) 11 1.362 1.365 0.00250 100.18% 0.721 189.14% 12 1.559 1.6160.05679 103.64% 0.721 224.02% 21 1.730 1.750 0.02005 101.16% 0.350500.05% 22 2.036 2.075 0.03887 101.91% 0.350 592.74% 31 2.165 2.1730.00823 100.38% 0.840 258.62% 32 2.260 2.322 0.06200 102.74% 0.840276.30% 41 2.427 2.683 0.25590 110.54% 0.779 344.54% 42 2.384 2.7290.34476 114.46% 0.779 350.46% 51 2.775 2.933 0.15796 105.69% 0.905323.93% 52 3.033 3.357 0.32327 110.66% 0.905 370.76% 61 3.108 3.4460.33766 110.86% 0.638 540.49% 62 3.954 4.236 0.28165 107.12% 0.638664.42%

The following contents may be deduced from Table 9 and Table 10.

Related inflection point values of fifth embodiment (Primary referencewavelength: 555 nm) HIF111 0.8584 HIF111/HOI 0.1717 SGI111 0.0449|SGI111|/(|SGI111| + TP1) 0.0586 HIF211 0.8458 HIF211/HOI 0.1692 SGI2110.0660 |SGI211|/(|SGI211| + TP2) 0.1587 HIF221 1.1017 HIF221/HOI 0.2203SGI221 0.1993 |SGI221|/(|SGI221| + TP2) 0.3628 HIF311 0.3554 HIF311/HOI0.0711 SGI311 0.0012 |SGI311|/(|SGI311| + TP3) 0.0014 HIF312 1.4302HIF312/HOI 0.2860 SGI312 −0.0267 |SGI312|/(|SGI312| + TP3) 0.0308 HIF3211.3245 HIF321/HOI 0.2649 SGI321 −0.2748 |SGI321|/(|SGI321| + TP3) 0.2464HIF322 2.0845 HIF322/HOI 0.4169 SGI322 −0.4063 |SGI322|/(|SGI322| + TP3)0.3259 HIF411 1.1851 HIF411/HOI 0.2370 SGI411 −0.4948|SGI411|/(|SGI411| + TP4) 0.3885 HIF421 1.5828 HIF421/HOI 0.3166 SGI421−0.7285 |SGI421|/(|SGI421| + TP4) 0.4833 HIF511 0.8018 HIF511/HOI 0.1604SGI511 0.0978 |SGI511|/(|SGI511| + TP5) 0.0975 HIF521 0.4059 HIF521/HOI0.0812 SGI521 −0.0126 |SGI521|/(|SGI521| + TP5) 0.0137 HIF522 1.1268HIF522/HOI 0.2254 SGI522 −0.0223 |SGI522|/(|SGI522| + TP5) 0.0240 HIF6110.1702 HIF611/HOI 0.0340 SGI611 −0.0003 |SGI611|/(|SGI611| + TP6) 0.0005HIF612 1.4252 HIF612/HOI 0.2850 SGI612 0.1127 |SGI612|/(|SGI612| + TP6)0.1502 HIF621 1.4439 HIF621/HOI 0.2888 SGI621 0.3200|SGI621|/(|SGI621| + TP6) 0.3342

The Sixth Embodiment (Embodiment 6)

Please refer to FIG. 6A, FIG. 6B and FIG. 6C, FIG. 6A is a schematicview of the optical image capturing system according to the sixthEmbodiment of the present application, FIG. 6B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the sixth Embodiment of the present application, andFIG. 6C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the sixth embodiment of the presentapplication. As shown in FIG. 6A, in order from an object side to animage side, the optical image capturing system includes a first lenselement 610, an aperture stop 600, a second lens element 620, a thirdlens element 630, a fourth lens element 640, a fifth lens element 650, asixth lens element 660, an IR-bandstop filter 680, an image plane 690,and an image sensing device 692.

The first lens element 610 has positive refractive power and it is madeof glass material. The first lens element 610 has a convex object-sidesurface 612 and a concave image-side surface 614, and both of theobject-side surface 612 and the image-side surface 614 are aspheric.

The second lens element 620 has negative refractive power and it is madeof glass material. The second lens element 620 has a concave object-sidesurface 622 and a convex image-side surface 624, and both of theobject-side surface 622 and the image-side surface 624 are aspheric.

The third lens element 630 has positive refractive power and it is madeof glass material. The third lens element 630 has a convex object-sidesurface 632 and a convex image-side surface 634, and both of theobject-side surface 632 and the image-side surface 634 are aspheric.

The fourth lens element 640 has positive refractive power and it is madeof glass material. The fourth lens element 640 has a concave object-sidesurface 642 and a convex image-side surface 644, and both of theobject-side surface 642 and the image-side surface 644 are aspheric. Theobject-side surface 642 has an inflection point.

The fifth lens element 650 has negative refractive power and it is madeof plastic material. The fifth lens element 650 has a concaveobject-side surface 652 and a concave image-side surface 654, and bothof the object-side surface 652 and the image-side surface 654 areaspheric. The image-side surface 654 has two inflection points.

The sixth lens element 660 has positive refractive power and it is madeof plastic material. The sixth lens element 660 has a convex object-sidesurface 662 and a concave image-side surface 664. The object-sidesurface 662 has three inflection points and the image-side surface 664has an inflection point. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 680 is made of plastic material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 660 and the image plane 690.

In the optical image capturing system of the sixth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=−40.244 mm andf1/ΣPP=0.287. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the sixth embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−45.248 mm andf2/ΣNP=0.852. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 11 and Table 12.

The detailed data of the optical image capturing system of the sixthEmbodiment is as shown in Table 11.

TABLE 11 Data of the optical image capturing system f = 4.215 mm; f/HEP= 1.7; HAF = 50.005 deg Focal Surface # Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Lens 15.254910129 0.437 Glass 1.743 44.95 11.552 2 12.90351667 0.094 3 Ape.Stop Plano 0.845 4 Lens 2 −2.043878685 0.416 Glass 1.753 29.71 −38.552 5−2.400649649 0.076 6 Lens 3 17.73602622 1.040 Glass 1.743 44.85 6.561 7−6.579105452 0.076 8 Lens 4 −26.59202214 0.889 Glass 1.743 44.85 9.694 9−5.757940799 1.061 10 Lens 5 −67.55563782 0.249 Plastic 1.621 24.48−6.696 11 4.479679028 0.193 12 Lens 6 7.636390669 0.314 Plastic 1.64222.46 12.437 13 136.4402377 0.094 14 IR-bandstop Plano 0.200 BK_7 1.51764.13 filter 15 Plano 1.263 16 Image Plano plane Reference wavelength(d-line) = 555 nmAs for the parameters of the aspheric surfaces of the sixth Embodiment,reference is made to Table 12.

TABLE 12 Aspheric Coefficients Surface # 1 2 4 5 6 7 k 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4−5.528163E−04 −5.544031E−04 −1.274861E−03 1.495805E−03 0.000000E+000.000000E+00 A6 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 A8 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 A10 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A12 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A140.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 Surface # 8 9 10 11 12 13 k 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A40.000000E+00 0.000000E+00 −2.885519E−02 −5.536360E−02 −3.948897E−022.180506E−03 A6 0.000000E+00 0.000000E+00 1.971379E−03 3.113405E−031.223805E−03 −6.950511E−04 A8 0.000000E+00 0.000000E+00 −1.336672E−041.671702E−04 3.012428E−04 6.126145E−05 A10 0.000000E+00 0.000000E+000.000000E+00 −1.368028E−05 −1.840965E−05 −1.870628E−06 A12 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A140.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00

In the sixth Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 11 and Table 12.

Sixth Embodiment (Primary reference wavelength: 555 nm) |f/f1| |f/f2||f/f3| |f/f4| |f/f5| |f/f6| 0.36486 0.10932 0.64242 0.43476 0.629390.33888 ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN56/f TP4/(IN34 + TP4 + IN45)1.78091 0.73871 2.41083 0.22322 0.04479 0.44755 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.29964 5.87626 3.32873 2.38081 HOS InTLHOS/HOI InS/HOS ODT % TDT % 7.24849 5.66114 1.44970 0.92608 2.002581.10761 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 0     1.070820.92508 1.17612 0.37522 0.25883 TP2/TP3 TP3/TP4 InRS61 InRS62|InRS61|/TP6 |InRS62|/TP6 0.39151 1.18471 −0.86294  −0.10165  2.670350.31456 PLTA PSTA NLTA NSTA SLTA SSTA −0.039 mm 0.029 mm 0.030 mm−0.00016 mm −0.046 mm −0.008 mm

The numerical related to the length of outline curve is shown accordingto table 11 and table 12.

Sixth embodiment (Reference wavelength = 555 nm) ARE ½(HEP) ARE valueARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.240 1.251 0.01095 100.88%0.437 285.92% 12 1.240 1.241 0.00123 100.10% 0.437 283.70% 21 1.2401.333 0.09301 107.50% 0.416 320.14% 22 1.240 1.300 0.06085 104.91% 0.416312.42% 31 1.240 1.240 0.00043 100.03% 1.040 119.29% 32 1.240 1.2460.00686 100.55% 1.040 119.90% 41 1.240 1.239 −0.00013 99.99% 0.889139.47% 42 1.240 1.249 0.00919 100.74% 0.889 140.52% 51 1.240 1.2430.00375 100.30% 0.249 499.82% 52 1.240 1.241 0.00173 100.14% 0.249499.01% 61 1.240 1.240 0.00041 100.03% 0.314 394.93% 62 1.240 1.239−0.00054 99.96% 0.314 394.63% ARS EHD ARS value ARS − EHD (ARS/EHD) % TPARS/TP (%) 11 1.479 1.499 0.01952 101.32% 0.437 342.65% 12 1.274 1.2750.00138 100.11% 0.437 291.50% 21 1.427 1.583 0.15545 110.89% 0.416380.20% 22 1.707 1.890 0.18364 110.76% 0.416 454.14% 31 2.554 2.5630.00856 100.34% 1.040 246.54% 32 2.649 2.725 0.07640 102.88% 1.040262.16% 41 2.762 2.766 0.00439 100.16% 0.889 311.25% 42 2.814 2.9390.12496 104.44% 0.889 330.71% 51 2.764 3.280 0.51647 118.69% 0.2491318.71% 52 3.154 3.368 0.21475 106.81% 0.249 1354.04% 61 3.234 3.4530.21867 106.76% 0.314 1099.69% 62 3.934 3.948 0.01472 100.37% 0.3141257.55%

The following contents may be deduced from Table 11 and Table 12.

Related inflection point values of sixth Embodiment (Primary referencewavelength: 555 nm) HIF411 1.6612 HIF411/HOI 0.3322 SGI411 −0.0477|SGI411|/(|SGI411| + TP4) 0.0503 HIF521 0.6006 HIF521/HOI 0.1201 SGI5210.0330 |SGI521|/(|SGI521| + TP5) 0.1331 HIF522 2.3654 HIF522/HOI 0.4731SGI522 −0.4310 |SGI522|/(|SGI522| + TP5) 0.6671 HIF611 0.5270 HIF611/HOI0.1054 SGI611 0.0147 |SGI611|/(|SGI611| + TP6) 0.0434 HIF612 2.3803HIF612/HOI 0.4761 SGI612 −0.4721 |SGI612|/(|SGI612| + TP6) 0.5937 HIF6133.0718 HIF613/HOI 0.6144 SGI613 −0.8509 |SGI613|/(|SGI613| + TP6) 0.7247HIF621 1.3381 HIF621/HOI 0.2676 SGI621 0.0061 |SGI621|/(|SGI621| + TP6)0.0185

The Seventh Embodiment (Embodiment 7)

Please refer to FIG. 7A, FIG. 7B and FIG. 7C, FIG. 7A is a schematicview of the optical image capturing system according to the seventhEmbodiment of the present application, FIG. 7B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the seventh Embodiment of the present application,and FIG. 7C is a lateral aberration diagram of tangential fan, sagittalfan, the longest operation wavelength and the shortest operationwavelength passing through an edge of the entrance pupil and incident onthe image plane by 0.7 HOI according to the seventh embodiment of thepresent application. As shown in FIG. 7A, in order from an object sideto an image side, the optical image capturing system includes a firstlens element 710, an aperture stop 700, a second lens element 720, athird lens element 730, a fourth lens element 740, a fifth lens element750, a sixth lens element 760, an IR-bandstop filter 780, an image plane790, and an image sensing device 792.

The first lens element 710 has positive refractive power and it is madeof plastic material. The first lens element 710 has a convex object-sidesurface 712 and a concave image-side surface 714, and both of theobject-side surface 712 and the image-side surface 714 are aspheric andhave an inflection point.

The second lens element 720 has negative refractive power and it is madeof plastic material. The second lens element 720 has a concaveobject-side surface 722 and a convex image-side surface 724, and both ofthe object-side surface 722 and the image-side surface 724 are asphericand have an inflection point.

The third lens element 730 has positive refractive power and it is madeof plastic material. The third lens element 730 has a concaveobject-side surface 732 and a convex image-side surface 734, and both ofthe object-side surface 732 and the image-side surface 734 are asphericand have an inflection point.

The fourth lens element 740 has positive refractive power and it is madeof plastic material. The fourth lens element 740 has a concaveobject-side surface 742 and a convex image-side surface 744, and both ofthe object-side surface 742 and the image-side surface 744 are asphericand have an inflection point.

The fifth lens element 750 has negative refractive power and it is madeof plastic material. The fifth lens element 750 has a concaveobject-side surface 752 and a concave image-side surface 754, and bothof the object-side surface 752 and the image-side surface 754 areaspheric and have an inflection point.

The sixth lens element 760 has positive refractive power and it is madeof plastic material. The sixth lens element 760 has a convex object-sidesurface 762 and a convex image-side surface 764. The object-side surface762 has an inflection point and the image-side surface 764 has twoinflection points. Hereby, the back focal length is reduced tominiaturize the lens element effectively. In addition, the angle ofincident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 780 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 760 and the image plane 790.

In the optical image capturing system of the seventh embodiment, a sumof focal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=57.669 mm andf1/ΣPP=0.131. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the seventh embodiment, a sumof focal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−91137.261 mm andf2/ΣNP=1. Hereby, it is favorable for allocating the negative refractivepower of a single lens element to other negative lens elements.

Please refer to the following Table 13 and Table 14.

The detailed data of the optical image capturing system of the seventhEmbodiment is as shown in Table 13.

TABLE 13 Data of the optical image capturing system f = 4.038 mm; f/HEP= 1.9; HAF = 50.008 deg Focal Surface # Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Lens 12.954518253 0.524 Plastic 1.642 22.46 7.546 2 6.950753966 0.128 3 Ape.Stop Plano 0.468 4 Lens 2 −3.644937036 0.368 Plastic 1.636 23.89−91133.200 5 −3.788729307 0.202 6 Lens 3 −46.68157182 0.664 Plastic1.642 22.46 4.316 7 −2.579313575 0.092 8 Lens 4 −3.309767187 0.811Plastic 1.544 55.96 40.186 9 −3.124437781 0.234 10 Lens 5 −4.5590231560.200 Plastic 1.584 29.88 −4.061 11 5.084571545 0.296 12 Lens 63.845208509 0.872 Plastic 1.642 22.46 5.621 13 −62.22261146 0.434 14IR-bandstop Plano 0.200 BK_7 1.517 64.13 filter 15 Plano 1.100 16 Imageplane Plano Reference wavelength (d-line) = 555 nmAs for the parameters of the aspheric surfaces of the seventhEmbodiment, reference is made to Table 14.

TABLE 14 Aspheric Coefficients Surface # 1 2 4 5 6 7 k 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4−6.145365E−03 −9.551903E−03 −1.260050E−01 −2.321729E−01 −2.260264E−01−6.707249E−02 A6 4.118407E−03 −1.713650E−03 4.607363E−02 1.551152E−011.651963E−01 3.134710E−02 A8 −3.343178E−03 −8.562003E−03 −1.505539E−02−4.034311E−02 −5.130555E−02 −2.240155E−03 A10 −7.899923E−04 2.413158E−031.189891E−02 7.480417E−03 6.104522E−03 −5.680731E−05 A12 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A140.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 A16 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 0.000000E+00 Surface # 8 9 10 11 12 13 k 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A4−6.329668E−02 −1.352471E−01 −1.636537E−01 −1.133064E−02 2.305982E−022.469605E−02 A6 1.474365E−02 4.171277E−02 6.201749E−02 −2.588320E−02−2.413549E−02 −6.920157E−03 A8 2.524026E−03 −5.153050E−03 −9.447310E−031.347575E−02 8.469079E−03 4.472012E−04 A10 −4.959290E−04 4.182142E−045.503487E−04 −3.873918E−03 −1.968813E−03 2.403706E−05 A12 0.000000E+000.000000E+00 0.000000E+00 6.404223E−04 2.502071E−04 −4.979119E−06 A140.000000E+00 0.000000E+00 0.000000E+00 −5.529044E−05 −1.528864E−052.942652E−07 A16 0.000000E+00 0.000000E+00 0.000000E+00 1.907356E−063.407612E−07 −7.051280E−09

In the seventh Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 13 and Table 14.

Seventh Embodiment (Primary reference wavelength: 555 nm) |f/f1| |f/f2||f/f3| |f/f4| |f/f5| |f/f6| 0.53516 0.00004 0.93563 0.10049 0.994430.71842 ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN56/f TP4/(IN34 + TP4 + IN45)2.28970 0.99447 2.30242 0.14752 0.07326 0.71340 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.00008 21115.1014    3.04543 5.84023 HOSInTL HOS/HOI InS/HOS ODT % TDT % 6.59156 4.85802 1.31831 0.90104 2.101620.95319 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 0     1.233541.89882 0.00000 0.00000 0.00000 TP2/TP3 TP3/TP4 InRS61 InRS62|InRS61|/TP6 |InRS62|/TP6 0.55372 0.81946 −0.37158  −0.57980  0.426010.66473 PLTA PSTA NLTA NSTA SLTA SSTA −0.030 mm 0.074 mm 0.095 mm 0.024mm −0.017 mm 0.038 mm

The numerical related to the length of outline curve is shown accordingto table 13 and table 14.

Seventh embodiment (Reference wavelength = 555 nm) ARE ½(HEP) ARE valueARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 1.063 1.084 0.02109 101.98%0.524 206.72% 12 1.063 1.064 0.00119 100.11% 0.524 202.93% 21 1.0631.106 0.04348 104.09% 0.368 300.78% 22 1.063 1.113 0.05002 104.71% 0.368302.56% 31 1.063 1.076 0.01336 101.26% 0.664 162.01% 32 1.063 1.1090.04679 104.40% 0.664 167.05% 41 1.063 1.098 0.03492 103.29% 0.811135.42% 42 1.063 1.126 0.06348 105.97% 0.811 138.95% 51 1.063 1.1100.04755 104.47% 0.200 555.12% 52 1.063 1.065 0.00257 100.24% 0.200532.63% 61 1.063 1.077 0.01420 101.34% 0.872 123.46% 62 1.063 1.062−0.00046 99.96% 0.872 121.78% ARS EHD ARS value ARS − EHD (ARS/EHD) % TPARS/TP (%) 11 1.399 1.435 0.03596 102.57% 0.524 273.80% 12 1.207 1.2090.00186 100.15% 0.524 230.59% 21 1.142 1.194 0.05231 104.58% 0.368324.72% 22 1.309 1.378 0.06881 105.26% 0.368 374.59% 31 1.630 1.6610.03107 101.91% 0.664 250.13% 32 1.809 1.945 0.13619 107.53% 0.664292.89% 41 1.933 2.056 0.12293 106.36% 0.811 253.66% 42 2.087 2.4550.36845 117.66% 0.811 302.89% 51 2.346 2.681 0.33527 114.29% 0.2001340.44% 52 2.773 3.112 0.33897 112.22% 0.200 1555.99% 61 3.046 3.4610.41513 113.63% 0.872 396.82% 62 3.642 3.901 0.25871 107.10% 0.872447.22%

The following contents may be deduced from Table 13 and Table 14.

Related inflection point values of seventh Embodiment (Primary referencewavelength: 555 nm) HIF111 1.1133 HIF111/HOI 0.2227 SGI111 0.2060|SGI111|/(|SGI111| + TP1) 0.2821 HIF121 0.7530 HIF121/HOI 0.1506 SGI1210.0368 |SGI121|/(|SGI121| + TP1) 0.0656 HIF211 1.0313 HIF211/HOI 0.2063SGI211 −0.2391 |SGI211|/(|SGI211| + TP2) 0.3940 HIF221 1.0026 HIF221/HOI0.2005 SGI221 −0.2456 |SGI221|/(|SGI221| + TP2) 0.4005 HIF311 1.0688HIF311/HOI 0.2138 SGI311 −0.1364 |SGI311|/(|SGI311| + TP3) 0.1704 HIF3211.2703 HIF321/HOI 0.2541 SGI321 −0.3932 |SGI321|/(|SGI321| + TP3) 0.3719HIF411 1.3327 HIF411/HOI 0.2665 SGI411 −0.3809 |SGI411|/(|SGI411| + TP4)0.3197 HIF421 1.5290 HIF421/HOI 0.3058 SGI421 −0.7306|SGI421|/(|SGI421| + TP4) 0.4741 HIF511 1.5093 HIF511/HOI 0.3019 SGI511−0.5938 |SGI511|/(|SGI511| + TP5) 0.7481 HIF521 0.7292 HIF521/HOI 0.1458SGI521 0.0464 |SGI521|/(|SGI521| + TP5) 0.1883 HIF611 1.2431 HIF611/HOI0.2486 SGI611 0.2065 |SGI611|/(|SGI611| + TP6) 0.1915 HIF621 0.2376HIF621/HOI 0.0475 SGI621 −0.0004 |SGI621|/(|SGI621| + TP6) 0.0004 HIF6221.3471 HIF622/HOI 0.2694 SGI622 0.0305 |SGI622|/(|SGI622| + TP6) 0.0338

The Eighth Embodiment (Embodiment 8)

Please refer to FIG. 8A, FIG. 8B and FIG. 8C, FIG. 8A is a schematicview of the optical image capturing system according to the eighthEmbodiment of the present application, FIG. 8B is longitudinal sphericalaberration curves, astigmatic field curves, and an optical distortioncurve of the optical image capturing system in the order from left toright according to the eighth Embodiment of the present application, andFIG. 8C is a lateral aberration diagram of tangential fan, sagittal fan,the longest operation wavelength and the shortest operation wavelengthpassing through an edge of the entrance pupil and incident on the imageplane by 0.7 HOI according to the eighth embodiment of the presentapplication. As shown in FIG. 8A, in order from an object side to animage side, the optical image capturing system includes an aperture stop800, a first lens element 810, a second lens element 820, a third lenselement 830, a fourth lens element 840, a fifth lens element 850, asixth lens element 860, an IR-bandstop filter 880, an image plane 890,and an image sensing device 892.

The first lens element 810 has positive refractive power and it is madeof plastic material. The first lens element 810 has a convex object-sidesurface 812 and a concave image-side surface 814, both of theobject-side surface 812 and the image-side surface 814 are aspheric, andthe image-side surface 814 has an inflection point.

The second lens element 820 has negative refractive power and it is madeof plastic material. The second lens element 820 has a concaveobject-side surface 822 and a concave image-side surface 824, and bothof the object-side surface 822 and the image-side surface 824 areaspheric. The image-side surface 824 has two inflection points.

The third lens element 830 has negative refractive power and it is madeof plastic material. The third lens element 830 has a convex object-sidesurface 832 and a concave image-side surface 834, and both of theobject-side surface 832 and the image-side surface 834 are aspheric. Theobject-side surface 832 and the image-side surface 834 both have aninflection point.

The fourth lens element 840 has positive refractive power and it is madeof plastic material. The fourth lens element 840 has a concaveobject-side surface 842 and a convex image-side surface 844, and both ofthe object-side surface 842 and the image-side surface 844 are aspheric.The object-side surface 842 has three inflection points.

The fifth lens element 850 has positive refractive power and it is madeof plastic material. The fifth lens element 850 has a convex object-sidesurface 852 and a convex image-side surface 854, and both of theobject-side surface 852 and the image-side surface 854 are aspheric. Theobject-side surface 852 has three inflection points and the image-sidesurface 854 has an inflection point.

The sixth lens element 860 has negative refractive power and it is madeof plastic material. The sixth lens element 860 has a concaveobject-side surface 862 and a concave image-side surface 864. Theobject-side surface 862 has two infection points and the image-sidesurface 864 has an inflection point. Hereby, the back focal length isreduced to miniaturize the lens element effectively. In addition, theangle of incident with incoming light from an off-axis view field can besuppressed effectively and the aberration in the off-axis view field canbe corrected further.

The IR-bandstop filter 880 is made of glass material without affectingthe focal length of the optical image capturing system and it isdisposed between the sixth lens element 860 and the image plane 890.

In the optical image capturing system of the eighth embodiment, a sum offocal lengths of all lens elements with positive refractive power isΣPP. The following relations are satisfied: ΣPP=12.785 mm andf5/ΣPP=0.10. Hereby, it is favorable for allocating the positiverefractive power of a single lens element to other positive lenselements and the significant aberrations generated in the process ofmoving the incident light can be suppressed.

In the optical image capturing system of the sixth embodiment, a sum offocal lengths of all lens elements with negative refractive power isΣNP. The following relations are satisfied: ΣNP=−112.117 mm andf6/ΣNP=0.009. Hereby, it is favorable for allocating the negativerefractive power of a single lens element to other negative lenselements.

Please refer to the following Table 15 and Table 16.

The detailed data of the optical image capturing system of the eighthEmbodiment is as shown in Table 15.

TABLE 15 Data of the optical image capturing system f = 3.213 mm; f/HEP= 2.4; HAF = 50.015 deg Focal Surface # Curvature Radius ThicknessMaterial Index Abbe # length 0 Object Plano At infinity 1 Shading Plano0.000 sheet 2 Ape. Stop Plano −0.108 3 Lens 1 2.117380565 0.267 Plastic1.565 58.00 6.003 4 5.351202213 0.632 5 Lens 2 −70.37596785 0.230Plastic 1.517 21.40 −11.326 6 8.30936549 0.050 7 Lens 3 7.3331718650.705 Plastic 1.565 58.00 −99.749 8 6.265499794 0.180 9 Lens 4−71.32533363 0.832 Plastic 1.565 58.00 5.508 10 −3.003657909 0.050 11Lens 5 3.397431079 0.688 Plastic 1.583 30.20 1.274 12 −0.886432266 0.05013 Lens 6 −3.715425702 0.342 Plastic 1.650 21.40 −1.042 14 0.8676236370.700 15 IR-bandstop Plano 0.200 1.517 64.13 filter 16 Plano 0.407 17Image plane Plano Reference wavelength (d-line) = 555 nm; shieldposition: clear aperture (CA) of the first plano = 0.640 mmAs for the parameters of the aspheric surfaces of the eighth Embodiment,reference is made to Table 16.

TABLE 16 Aspheric Coefficients Surface # 3 4 5 6 7 8 k −1.486403E+002.003790E+01 −4.783682E+01 −2.902431E+01 −5.000000E+01 −5.000000E+01 A42.043654E−02 −2.642626E−02 −6.237485E−02 −4.896336E−02 −7.363667E−02−5.443257E−02 A6 −2.231403E−04 −4.147746E−02 −8.137705E−02 −1.981368E−021.494245E−02 1.263891E−04 A8 −1.387235E−02 2.901026E−02 4.589961E−023.312952E−03 6.252296E−03 −9.655324E−03 A10 −3.431740E−02 −9.512960E−02−5.485574E−02 5.634445E−03 −2.226544E−03 1.318692E−03 A12 0.000000E+000.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 A140.000000E+00 0.000000E+00 0.000000E+00 0.000000E+00 0.000000E+000.000000E+00 Surface # 9 10 11 12 13 14 k −5.000000E+01 8.520005E−01−5.000000E+01 −4.524978E+00 −5.000000E+01 −4.286435E+00 A4 3.105497E−02−6.786287E−03 −9.520247E−02 −4.666187E−02 5.856863E−03 −2.635938E−02 A6−1.532514E−02 6.693976E−03 −5.507560E−05 3.849227E−03 2.442214E−033.694093E−03 A8 −6.443603E−04 8.220809E−04 1.932773E−03 1.041053E−03−2.201034E−03 −1.355873E−04 A10 4.321089E−04 −2.798394E−04 3.346274E−044.713339E−06 −1.065215E−04 −5.321575E−05 A12 0.000000E+00 0.000000E+001.125736E−05 −2.834871E−06 1.227641E−04 6.838440E−06 A14 0.000000E+000.000000E+00 −1.671951E−05 −2.293810E−06 −1.181115E−05 −2.530792E−07

In the eighth Embodiment, the presentation of the aspheric surfaceformula is similar to that in the first embodiment. Besides, thedefinitions of parameters in following tables are equal to those in thefirst embodiment, so the repetitious details will not be given here.

The following contents may be deduced from Table 15 and Table 16.

Eighth Embodiment (Primary reference wavelength: 555 nm) |f/f1| |f/f2||f/f3| |f/f4| |f/f5| |f/f6| 0.53529 0.28371 0.03221 0.58335 2.521393.08263 ΣPPR ΣNPR ΣPPR/|ΣNPR| IN12/f IN56/f TP4/(IN34 + TP4 + IN45)6.72266 0.84594 7.94700 0.19680 0.01556 0.78362 |f1/f2| |f2/f3| (TP1 +IN12)/TP2 (TP6 + IN56)/TP5 0.53001 0.11354 3.90947 0.56888 HOS InTLHOS/HOI InS/HOS ODT % TDT % 5.33002 4.02576 1.36178 0.97981 1.923711.09084 HVT51 HVT52 HVT61 HVT62 HVT62/HOI HVT62/HOS 0.67483 0    0.00000 2.23965 0.57222 0.42020 TP2/TP3 TP3/TP4 InRS61 InRS62|InRS61|/TP6 |InRS62|/TP6 0.32631 0.84713 −0.74088  −0.06065  2.168960.17755 PLTA PSTA NLTA NSTA SLTA SSTA 0.005 mm −0.003 mm 0.010 mm 0.006mm 0.004 mm 0.003 mm

The numerical related to the length of outline curve is shown accordingto table 15 and table 16.

Eighth embodiment (Primary reference wavelength = 555 nm) ARE ½(HEP) AREvalue ARE − ½(HEP) 2(ARE/HEP) % TP ARE/TP (%) 11 0.648 0.658 0.01023101.58% 0.267 246.73% 12 0.670 0.670 0.00041 100.06% 0.267 251.19% 210.670 0.670 0.00002 100.00% 0.230 291.24% 22 0.670 0.669 −0.00064 99.90%0.230 290.95% 31 0.670 0.669 −0.00063 99.91% 0.705 94.94% 32 0.670 0.669−0.00046 99.93% 0.705 94.97% 41 0.670 0.669 −0.00082 99.88% 0.832 80.40%42 0.670 0.675 0.00511 100.76% 0.832 81.12% 51 0.670 0.670 −0.00003100.00% 0.688 97.31% 52 0.670 0.702 0.03243 104.84% 0.688 102.02% 610.670 0.671 0.00099 100.15% 0.342 196.39% 62 0.670 0.699 0.02890 104.31%0.342 204.56% ARS EHD ARS value ARS − EHD (ARS/EHD) % TP ARS/TP (%) 110.648 0.658 0.01023 101.58% 0.267 246.73% 12 0.697 0.697 0.00042 100.06%0.267 261.33% 21 0.994 1.026 0.03192 103.21% 0.230 446.16% 22 1.2551.259 0.00315 100.25% 0.230 547.21% 31 1.383 1.385 0.00192 100.14% 0.705196.48% 32 1.604 1.816 0.21279 113.27% 0.705 257.68% 41 1.876 1.9080.03181 101.70% 0.832 229.32% 42 2.027 2.193 0.16648 108.21% 0.832263.61% 51 2.038 2.282 0.24376 111.96% 0.688 331.49% 52 2.144 2.4850.34081 115.89% 0.688 361.03% 61 2.411 2.624 0.21261 108.82% 0.342768.18% 62 3.309 3.686 0.37664 111.38% 0.342 1078.99%

The following contents may be deduced from Table 15 and Table 16.

Related inflection point values of eighth Embodiment (Primary referencewavelength: 555 nm) HIF121 0.57452 HIF121/HOI 0.14679 SGI121 0.02858|SGI121|/(|SGI121| + TP1) 0.09675 HIF221 0.40206 HIF221/HOI 0.10272SGI221 0.00821 |SGI221|/(|SGI221| + TP2) 0.03448 HIF222 1.11769HIF222/HOI 0.28556 SGI222 −0.02234 |SGI222|/(|SGI222| + TP2) 0.08853HIF311 0.37391 HIF311/HOI 0.09553 SGI311 0.00785 |SGI311|/(|SGI311| +TP3) 0.01102 HIF321 0.42061 HIF321/HOI 0.10746 SGI321 0.01170|SGI321|/(|SGI321| + TP3) 0.01633 HIF411 0.19878 HIF411/HOI 0.05079SGI411 −0.00023 |SGI411|/(|SGI411| + TP4) 0.00028 HIF412 0.87349HIF412/HOI 0.22317 SGI412 0.00583 |SGI412|/(|SGI412| + TP4) 0.00695HIF413 1.87638 HIF413/HOI 0.47940 SGI413 −0.17360 |SGI413|/(|SGI413| +TP4) 0.17263 HIF511 0.36373 HIF511/HOI 0.09293 SGI511 0.015644|SGI511|/(|SGI511| + TP5) 0.02222 HIF512 1.7159 HIF512/HOI 0.43840SGI512 −0.446747 |SGI512|/(|SGI512| + TP5) 0.39358 HIF513 1.93653HIF513/HOI 0.49477 SGI513 −0.638544 |SGI513|/(|SGI513| + TP5) 0.48124HIF521 1.54767 HIF521/HOI 0.39542 SGI521 −0.792114 |SGI521|/(|SGI521| +TP5) 0.53505 HIF611 0.82168 HIF611/HOI 0.20993 SGI611 −0.060958|SGI611|/(|SGI611| + TP6) 0.15143 HIF612 0.98146 HIF612/HOI 0.25076SGI612 −0.07785 |SGI612|/(|SGI612| + TP6) 0.18561 HIF621 0.79476HIF621/HOI 0.20306 SGI621 0.238143 |SGI621|/(|SGI621| + TP6) 0.41079

The above-mentioned descriptions represent merely the exemplaryembodiment of the present disclosure, without any intention to limit thescope of the present disclosure thereto. Various equivalent changes,alternations or modifications based on the claims of present disclosureare all consequently viewed as being embraced by the scope of thepresent disclosure.

What is claimed is:
 1. An optical image capturing system, from an objectside to an image side, comprising: a first lens element with refractivepower; a second lens element with refractive power; a third lens elementwith refractive power; a fourth lens element with refractive power; afifth lens element with refractive power; a sixth lens element withrefractive power; and an image plane; wherein the optical imagecapturing system consists of the six lens elements with refractivepower, a maximum height for image formation on the image planeperpendicular to the optical axis in the optical image capturing systemis denoted by HOI, at least one of the first through sixth lens elementshas positive refractive power, focal lengths of the first through sixthlens elements are f1, f2, f3, f4, f5 and f6 respectively, a focal lengthof the optical image capturing system is f, an entrance pupil diameterof the optical image capturing system is HEP, a distance on an opticalaxis from an object-side surface of the first lens element to the imageplane is HOS, a distance on an optical axis from the object-side surfaceof the first lens element to the image-side surface of the sixth lenselement is InTL, a length of outline curve from an axial point on anysurface of any one of the six lens elements to a coordinate point ofvertical height with a distance of a half of the entrance pupil diameterfrom the optical axis on the surface along an outline of the surface isdenoted as ARE, and the following relations are satisfied:1.2≦f/HEP≦3.0, 0<InTL/HOS<0.9 and 0.9≦2(ARE/HEP)≦1.5, wherein a half ofa maximum view angle of the optical image capturing system is HAF, andthe following relation is satisfied: 0 deg<HAF≦60 deg, and wherein thefollowing relation is satisfied: 0 mm<HOS≦30 mm.
 2. The optical imagecapturing system of claim 1, wherein TV distortion for image formationin the optical image capturing system is TDT, a maximum height for imageformation on the image plane perpendicular to the optical axis in theoptical image capturing system is denoted by HOI, a lateral aberrationof the longest operation wavelength of a visible light of a positivedirection tangential fan of the optical image capturing system passingthrough an edge of the entrance pupil and incident on the image plane by0.7 HOI is denoted as PLTA, and a lateral aberration of the shortestoperation wavelength of a visible light of the positive directiontangential fan of the optical image capturing system passing through theedge of the entrance pupil and incident on the image plane by 0.7 HOI isdenoted as PSTA, a lateral aberration of the longest operationwavelength of a visible light of a negative direction tangential fan ofthe optical image capturing system passing through the edge of theentrance pupil and incident on the image plane by 0.7 HOI is denoted asNLTA, a lateral aberration of the shortest operation wavelength of avisible light of a negative direction tangential fan of the opticalimage capturing system passing through the edge of the entrance pupiland incident on the image plane by 0.7 HOI is denoted as NSTA, a lateralaberration of the longest operation wavelength of a visible light of asagittal fan of the optical image capturing system passing through theedge of the entrance pupil and incident on the image plane by 0.7 HOI isdenoted as SLTA, a lateral aberration of the shortest operationwavelength of a visible light of the sagittal fan of the optical imagecapturing system passing through the edge of the entrance pupil andincident on the image plane by 0.7 HOI is denoted as SSTA, and thefollowing relations are satisfied: PLTA≦100 μm; PSTA≦100 μm; NLTA≦100μm; NSTA≦100 μm; SLTA≦100 μm; and SSTA≦100 μm; |TDT|<250%.
 3. Theoptical image capturing system of claim 1, wherein a maximum effectivehalf diameter position of any surface of any one of the six lenselements is denoted as EHD, and a length of outline curve from an axialpoint on any surface of any one of the six lens elements to the maximumeffective half diameter position of the surface along the outline of thesurface is denoted as ARE, and the following relation is satisfied:0.9≦ARS/EHD≦2.0.
 4. The optical image capturing system of claim 1,wherein a length of outline curve from an axial point on the object-sidesurface of the sixth lens element to a coordinate point of verticalheight with a distance of a half of the entrance pupil diameter from theoptical axis on the surface along an outline of the surface is denotedas ARE61; a length of outline curve from an axial point on theimage-side surface of the sixth lens element to the coordinate point ofvertical height with the distance of a half of the entrance pupildiameter from the optical axis on the surface along the outline of thesurface is denoted as ARE62, and a thickness of the sixth lens elementon the optical axis is TP6, and the following relations are satisfied:0.05≦ARE61/TP6≦20, and 0.05≦ARE62/TP6≦20.
 5. The optical image capturingsystem of claim 1, wherein a length of outline curve from an axial pointon the object-side surface of the fifth lens element to a coordinatepoint of vertical height with a distance of a half of the entrance pupildiameter from the optical axis on the surface along an outline of thesurface is denoted as ARE51; a length of outline curve from an axialpoint on the image-side surface of the fifth lens element to thecoordinate point of vertical height with the distance of a half of theentrance pupil diameter from the optical axis on the surface along theoutline of the surface is denoted as ARE52, and a thickness of the fifthlens element on the optical axis is TP5, and the following relations aresatisfied: 0.05≦ARE51/TP5≦20; and 0.05≦ARE52/TP5≦20.
 6. The opticalimage capturing system of claim 1, wherein the first lens element has apositive refractive power and the second lens element has a negativerefractive power.
 7. The optical image capturing system of claim 1,further comprising an aperture stop, a distance from the aperture stopto the image plane on the optical axis is InS, and the followingrelation is satisfied: 0.2≦InS/HOS≦1.1.
 8. An optical image capturingsystem, from an object side to an image side, comprising: a first lenselement with positive refractive power; a second lens element withrefractive power; a third lens element with refractive power; a fourthlens element with refractive power; a fifth lens element with refractivepower; a sixth lens element with refractive power; and an image plane;wherein the optical image capturing system consists of the six lenselements with refractive power, a maximum height for image formation onthe image plane perpendicular to the optical axis in the optical imagecapturing system is denoted by HOI, at least two lens elements among thefirst through sixth lens elements respectively have at least oneinflection point on at least one surface thereof, at least one of thesecond through sixth lens elements has positive refractive power, focallengths of the first through sixth lens elements are f1, f2, f3, f4, f5and f6 respectively, a focal length of the optical image capturingsystem is f, an entrance pupil diameter of the optical image capturingsystem is HEP, a distance on an optical axis from an object-side surfaceof the first lens element to the image plane is HOS, a distance on anoptical axis from the object-side surface of the first lens element tothe image-side surface of the sixth lens element is InTL, a length ofoutline curve from an axial point on any surface of any one of the sixlens elements to a coordinate point of vertical height with a distanceof a half of the entrance pupil diameter from the optical axis on thesurface along an outline of the surface is denoted as ARE, and thefollowing relations are satisfied: 1.2≦f/HEP≦3.0, 0<InTL/HOS<0.9 and0.9≦2(ARE/HEP)≦1.5, wherein a half of a maximum view angle of theoptical image capturing system is HAF, and the following relation issatisfied: 0 deg<HAF≦60 deg.
 9. The optical image capturing system ofclaim 8, wherein a maximum effective half diameter position of anysurface of any one of the six lens elements is denoted as EHD, and alength of outline curve from an axial point on any surface of any one ofthe six lens elements to the maximum effective half diameter position ofthe surface along the outline of the surface is denoted as ARS, and thefollowing relation is satisfied: 0.9≦ARS/EHD≦2.0.
 10. The optical imagecapturing system of claim 8, wherein at least three lens elements amongthe first through sixth lens elements respectively have at least oneinflection point on at least one surface thereof.
 11. The optical imagecapturing system of claim 8, wherein a maximum height for imageformation on the image plane perpendicular to the optical axis in theoptical image capturing system is denoted by HOI, a lateral aberrationof the longest operation wavelength of a visible light of a positivedirection tangential fan of the optical image capturing system passingthrough an edge of the entrance pupil and incident on the image plane by0.7 HOI is denoted as PLTA, and a lateral aberration of the shortestoperation wavelength of a visible light of the positive directiontangential fan of the optical image capturing system passing through theedge of the entrance pupil and incident on the image plane by 0.7 HOI isdenoted as PSTA, a lateral aberration of the longest operationwavelength of a visible light of a negative direction tangential fan ofthe optical image capturing system passing through the edge of theentrance pupil and incident on the image plane by 0.7 HOI is denoted asNLTA, a lateral aberration of the shortest operation wavelength of avisible light of a negative direction tangential fan of the opticalimage capturing system passing through the edge of the entrance pupiland incident on the image plane by 0.7 HOI is denoted as NSTA, a lateralaberration of the longest operation wavelength of a visible light of asagittal fan of the optical image capturing system passing through theedge of the entrance pupil and incident on the image plane by 0.7 HOI isdenoted as SLTA, a lateral aberration of the shortest operationwavelength of a visible light of the sagittal fan of the optical imagecapturing system passing through the edge of the entrance pupil andincident on the image plane by 0.7 HOI is denoted as SSTA, and thefollowing relations are satisfied: PLTA≦100 μm; PSTA≦100 μm; NLTA≦100μm; NSTA≦100 μm; SLTA 100 μm; SSTA≦100 μm and HOI>3.0 mm.
 12. Theoptical image capturing system of claim 8, wherein at least one of thefirst, the second, the third, the fourth, the fifth and the sixth lenselements is a light filtration element with a wavelength of less than500 nm.
 13. The optical image capturing system of claim 8, wherein adistance between the first lens element and the second lens element onthe optical axis is IN12, and the following relation is satisfied:0<IN12/f≦3.0.
 14. The optical image capturing system of claim 8, whereina distance between the fifth lens element and the sixth lens element onthe optical axis is IN56, and the following relation is satisfied:0<IN56/f≦0.8.
 15. The optical image capturing system of claim 8, whereinthe distance from the fifth lens element to the sixth lens element onthe optical axis is IN56, a thickness of the fifth lens element and athickness of the sixth lens element on the optical axis respectively areTP5 and TP6, and the following relation is satisfied:0.1≦(TP6+IN56)/TP5≦10.
 16. The optical image capturing system of claim8, wherein the distance from the first lens element to the second lenselement on the optical axis is IN12, a thickness of the first lenselement and a thickness of the second lens element on the optical axisrespectively are TP1 and TP2, and the following relation is satisfied:0.1≦(TP1+IN12)/TP2≦10.
 17. The optical image capturing system of claim8, wherein a distance from the third lens element to the fourth lenselement on the optical axis is IN34, a distance from the fourth lenselement to the fifth lens element on the optical axis is IN45, athickness of the fourth lens element is TP4, and the following relationis satisfied: 0<TP4/(IN34+TP4+IN45)<1.
 18. An optical image capturingsystem, from an object side to an image side, comprising: a first lenselement with positive refractive power; a second lens element withnegative refractive power; a third lens element with refractive power; afourth lens element with refractive power; a fifth lens element withrefractive power; a sixth lens element with refractive power; and animage plane; wherein the optical image capturing system consists of thesix lens elements with refractive power, a maximum height for imageformation on the image plane perpendicular to the optical axis in theoptical image capturing system is denoted by HOI, at least three lenselements among the first through sixth lens elements respectively haveat least one inflection point on at least one surface thereof, anobject-side surface and an image-side surface of at least one of the sixlens elements are aspheric, focal lengths of the first through sixthlens elements are f1, f2, f3, f4, f5 and f6 respectively, a focal lengthof the optical image capturing system is f, an entrance pupil diameterof the optical image capturing system is HEP, a half of maximum viewangle of the optical image capturing system is HAF, a distance on anoptical axis from an object-side surface of the first lens element tothe image plane is HOS, a distance on an optical axis from theobject-side surface of the first lens element to the image-side surfaceof the sixth lens element is InTL, a length of outline curve from anaxial point on any surface of any one of the six lens elements to acoordinate point of vertical height with a distance of a half of theentrance pupil diameter from the optical axis on the surface along anoutline of the surface is denoted as ARE, and the following relationsare satisfied: 1.2≦f/HEP≦3.0; 0.4≦| tan(HAF)|≦1.5; 0<InTL/HOS<0.9;HOI>3.0 mm and 0.9≦2(ARE/HEP)≦1.5, wherein a length of outline curvefrom an axial point on the object-side surface of the sixth lens elementto a coordinate point of vertical height with a distance of a half ofthe entrance pupil diameter from the optical axis on the surface alongan outline of the surface is denoted as ARE61; a length of outline curvefrom an axial point on the image-side surface of the sixth lens elementto the coordinate point of vertical height with the distance of a halfof the entrance pupil diameter from the optical axis on the surfacealong the outline of the surface is denoted as ARE62, and a thickness ofthe sixth lens element on the optical axis is TP6, and the followingrelations are satisfied: 0.05≦ARE61/TP6≦20 and 0.05≦ARE62/TP6≦20. 19.The optical image capturing system of claim 18, wherein a maximumeffective half diameter position of any surface of any one of the sixlens elements is denoted as EHD, and a length of outline curve from anaxial point on any surface of any one of the six lens elements to themaximum effective half diameter position of the surface along theoutline of the surface is denoted as ARS, and the following relation issatisfied: 0.9≦ARS/EHD≦2.0.
 20. The optical image capturing system ofclaim 18, wherein the following relation is satisfied: 0 mm<HOS≦30 mm.21. The optical image capturing system of claim 18, wherein a length ofoutline curve from an axial point on the object-side surface of thefifth lens element to a coordinate point of vertical height with adistance of a half of the entrance pupil diameter from the optical axison the surface along an outline of the surface is denoted as ARE51; alength of outline curve from an axial point on the image-side surface ofthe fifth lens element to the coordinate point of vertical height withthe distance of a half of the entrance pupil diameter from the opticalaxis on the surface along the outline of the surface is denoted asARE52, and a thickness of the fifth lens element on the optical axis isTP5, and the following relations are satisfied: 0.05≦ARE51/TP5≦20 and0.05≦ARE52/TP5≦20.
 22. The optical image capturing system of claim 18,wherein the optical image capturing system further comprise an aperturestop, an image sensing device and a driving module, the image sensingdevice is disposed on the image plane, a distance from the aperture stopto the image plane is InS, and the driving module couples with the lenselements to displace the lens elements, and the following relation issatisfied: 0.2≦InS/HOS≦1.1.